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| Boilerpipe Text | From Wikipedia, the free encyclopedia
In
string theory
, the
string theory landscape
(or
landscape of vacua
) is the collection of possible
false vacua
,
[
1
]
together comprising a collective "landscape" of choices of parameters governing
compactifications
.
The term "landscape" comes from the notion of a
fitness landscape
in
evolutionary biology
.
[
2
]
It was first applied to cosmology by
Lee Smolin
in his book
The Life of the Cosmos
(1997), and was first used in the context of string theory by
Leonard Susskind
.
[
3
]
Compactified Calabi–Yau manifolds
[
edit
]
In string theory, the estimated count of distinct flux vacua is commonly stated as having a lower bound of
,
[
4
]
but more recently this has been revised to
,
[
5
]
and the true number may still be far higher. The large number of possibilities arises from choices of
Calabi–Yau manifolds
and choices of generalized
magnetic fluxes
over various
homology
cycles, found in
F-theory
.
If there is no structure in the space of vacua, the problem of finding one with a sufficiently small cosmological constant is
NP complete
.
[
6
]
This is a version of the
subset sum problem
.
A possible mechanism of string theory vacuum stabilization, now known as the
KKLT mechanism
, was proposed in 2003 by
Shamit Kachru
,
Renata Kallosh
,
Andrei Linde
, and
Sandip Trivedi
.
[
7
]
Fine-tuning by the anthropic principle
[
edit
]
Fine-tuning
of constants like the
cosmological constant
or the
Higgs boson
mass is usually assumed to occur for precise physical reasons as opposed to taking their particular values at random. That is, these values should be uniquely consistent with underlying physical laws.
The number of theoretically allowed configurations has prompted suggestions
[
according to whom?
]
that this is not the case, and that many different vacua are physically realized.
[
8
]
The
anthropic principle
proposes that fundamental constants may have the values they have because such values are necessary for life (and therefore intelligent observers to measure the constants). The
anthropic landscape
thus refers to the collection of those portions of the landscape that are suitable for supporting intelligent life.
In 1987,
Steven Weinberg
proposed that the observed value of the
cosmological constant
was so small because it is impossible for life to occur in a universe with a much larger cosmological constant.
[
9
]
Weinberg attempted to predict the magnitude of the cosmological constant based on probabilistic arguments. Other attempts
[
which?
]
have been made to apply similar reasoning to models of particle physics.
[
10
]
Such attempts are based in the general ideas of
Bayesian probability
; interpreting probability in a context where it is only possible to draw one
sample
from a
distribution
is problematic in
frequentist probability
but not in Bayesian probability, which is not defined in terms of the frequency of repeated events.
In such a framework, the probability
of observing some fundamental parameters
is given by,
where
is the prior probability, from fundamental theory, of the parameters
and
is the "anthropic selection function", determined by the number of "observers" that would occur in the universe with parameters
.
[
citation needed
]
These probabilistic arguments are the most controversial aspect of the landscape. Technical criticisms of these proposals have pointed out that:
[
citation needed
]
[
year needed
]
The function
is completely unknown in string theory and may be impossible to define or interpret in any sensible probabilistic way.
The function
is completely unknown, since so little is known about the origin of life. Simplified criteria (such as the number of galaxies) must be used as a proxy for the number of observers. Moreover, it may never be possible to compute it for parameters radically different from those of the observable universe.
Simplified approaches
[
edit
]
Tegmark
et al.
have recently considered these objections and proposed a simplified anthropic scenario for
axion
dark matter
in which they argue that the first two of these problems do not apply.
[
11
]
Vilenkin and collaborators have proposed a consistent way to define the probabilities for a given vacuum.
[
12
]
A problem with many of the simplified approaches people
[
who?
]
have tried is that they "predict" a cosmological constant that is too large by a factor of 10–1000 orders of magnitude (depending on one's assumptions) and hence suggest that the cosmic acceleration should be much more rapid than is observed.
[
13
]
[
14
]
[
15
]
Few dispute the large number of metastable vacua.
[
citation needed
]
The existence, meaning, and scientific relevance of the anthropic landscape, however, remain controversial.
[
further explanation needed
]
Cosmological constant problem
[
edit
]
Andrei Linde
,
Sir Martin Rees
and
Leonard Susskind
advocate it as a solution to the
cosmological constant problem
.
[
citation needed
]
Weak scale supersymmetry from the landscape
[
edit
]
The string landscape ideas can be applied to the notion of weak scale supersymmetry and the Little Hierarchy problem.
For string vacua which include the MSSM (Minimal Supersymmetric Standard Model) as the low energy effective field theory, all values of SUSY breaking fields
are expected to be equally likely on the landscape. This led Douglas
[
16
]
and others to propose that the SUSY breaking scale is distributed as a power
law in the landscape
where
is the number of F-breaking fields
(distributed as complex numbers) and
is the number of D-breaking fields (distributed as real numbers).
Next, one may impose the Agrawal, Barr, Donoghue, Seckel (ABDS) anthropic requirement
[
17
]
that the derived weak scale lie within a factor of a few
of our measured value (lest nuclei as needed for life as we know it become unstable (the atomic principle)).
Combining these effects with a mild power-law draw to large soft SUSY breaking terms,
one may calculate the Higgs boson and superparticle masses expected from the landscape.
[
18
]
The Higgs mass probability distribution peaks around 125 GeV while sparticles (with the exception of light higgsinos) tend to
lie well beyond current LHC search limits. This approach is an example of the application of stringy naturalness.
Scientific relevance
[
edit
]
David Gross
suggests
[
citation needed
]
that the idea is inherently unscientific, unfalsifiable or premature. A famous debate on the anthropic landscape of string theory is the
Smolin–Susskind debate
on the merits of the landscape.
There are several popular books about the anthropic principle in cosmology.
[
19
]
The authors of two physics blogs,
Lubos Motl
and
Peter Woit
, are opposed to this use of the anthropic principle.
[
why?
]
[
20
]
Swampland
Extra dimensions
M-theory
^
The number of metastable vacua is not known exactly, but commonly quoted estimates are of the order 10
500
. See
M. Douglas
, "The statistics of string / M theory vacua",
JHEP
0305
, 46 (2003).
arXiv
:
hep-th/0303194
; S. Ashok and M. Douglas, "Counting flux vacua",
JHEP
0401
, 060 (2004).
^
Baggott, Jim (2018).
Quantum Space Loop Quantum Gravity and the Search for the Structure of Space, Time, and the Universe
. Oxford University Press. p. 288.
ISBN
978-0-19-253681-5
.
^
L. Smolin, "Did the universe evolve?",
Classical and Quantum Gravity
9
, 173–191 (1992). L. Smolin,
The Life of the Cosmos
(Oxford, 1997)
^
Read, James; Le Bihan, Baptiste (2021).
"The landscape and the multiverse: What's the problem?"
.
Synthese
.
199
(
3–
4):
7749–
7771.
doi
:
10.1007/s11229-021-03137-0
.
S2CID
234815857
.
^
Taylor, Washington; Wang, Yi-Nan (2015). "The F-theory geometry with most flux vacua".
Journal of High Energy Physics
.
2015
(12): 164.
arXiv
:
1511.03209
.
Bibcode
:
2015JHEP...12..164T
.
doi
:
10.1007/JHEP12(2015)164
.
S2CID
41149049
.
^
Frederik Denef; Douglas, Michael R. (2007). "Computational complexity of the landscape".
Annals of Physics
.
322
(5):
1096–
1142.
arXiv
:
hep-th/0602072
.
Bibcode
:
2007AnPhy.322.1096D
.
doi
:
10.1016/j.aop.2006.07.013
.
S2CID
281586
.
^
Kachru, Shamit; Kallosh, Renata; Linde, Andrei; Trivedi, Sandip P. (2003). "de Sitter Vacua in String Theory".
Physical Review D
.
68
(4) 046005.
arXiv
:
hep-th/0301240
.
Bibcode
:
2003PhRvD..68d6005K
.
doi
:
10.1103/PhysRevD.68.046005
.
S2CID
119482182
.
^
L. Susskind, "The anthropic landscape of string theory",
arXiv
:
hep-th/0302219
.
^
S. Weinberg, "Anthropic bound on the cosmological constant",
Phys. Rev. Lett.
59
, 2607 (1987).
^
S. M. Carroll, "Is our universe natural?" (2005)
arXiv
:
hep-th/0512148
reviews a number of proposals in preprints dated 2004/5.
^
M. Tegmark, A. Aguirre, M. Rees and F. Wilczek, "Dimensionless constants, cosmology and other dark matters",
arXiv
:
astro-ph/0511774
. F. Wilczek, "Enlightenment, knowledge, ignorance, temptation",
arXiv
:
hep-ph/0512187
. See also the discussion at
[1]
.
^
See,
e.g.
Alexander Vilenkin (2007). "A measure of the multiverse".
Journal of Physics A: Mathematical and Theoretical
.
40
(25):
6777–
6785.
arXiv
:
hep-th/0609193
.
Bibcode
:
2007JPhA...40.6777V
.
doi
:
10.1088/1751-8113/40/25/S22
.
S2CID
119390736
.
^
Abraham Loeb (2006). "An observational test for the anthropic origin of the cosmological constant".
Journal of Cosmology and Astroparticle Physics
.
0605
(5): 009.
arXiv
:
astro-ph/0604242
.
Bibcode
:
2006JCAP...05..009L
.
doi
:
10.1088/1475-7516/2006/05/009
.
S2CID
39340203
.
^
Jaume Garriga & Alexander Vilenkin (2006). "Anthropic prediction for Lambda and the Q catastrophe".
Prog. Theor. Phys. Suppl
.
163
:
245–
57.
arXiv
:
hep-th/0508005
.
Bibcode
:
2006PThPS.163..245G
.
doi
:
10.1143/PTPS.163.245
.
S2CID
118936307
.
^
Delia Schwartz-Perlov & Alexander Vilenkin (2006). "Probabilities in the Bousso-Polchinski multiverse".
Journal of Cosmology and Astroparticle Physics
.
0606
(6): 010.
arXiv
:
hep-th/0601162
.
Bibcode
:
2006JCAP...06..010S
.
doi
:
10.1088/1475-7516/2006/06/010
.
S2CID
119337679
.
^
M. R. Douglas, "Statistical analysis of the supersymmetry breaking scale",
arXiv
:
hep-th/0405279
.
^
V. Agrawal, S. M. Barr, J. F. Donoghue and
D. Seckel, "Anthropic considerations in multiple domain theories and the scale of electroweak symmetry breaking",
Phys. Rev. Lett.
80
, 1822 (1998).
arXiv
:
hep-ph/9801253
^
H. Baer, V. Barger, H. Serce and K. Sinha, "Higgs and superparticle mass predictions from the landscape",
JHEP
03
, 002 (2018),
arXiv
:
1712.01399
.
^
L. Susskind,
The cosmic landscape: string theory and the illusion of intelligent design
(Little, Brown, 2005). M. J. Rees,
Just six numbers: the deep forces that shape the universe
(Basic Books, 2001). R. Bousso and J. Polchinski, "The string theory landscape",
Sci. Am.
291
, 60–69 (2004).
^
Motl's blog criticized the anthropic principle and Woit's
blog
frequently attacks the anthropic string landscape.
String landscape; moduli stabilization; flux vacua; flux compactification
on
arxiv.org
.
Cvetič, Mirjam
; García-Etxebarria, Iñaki; Halverson, James (March 2011). "On the computation of non-perturbative effective potentials in the string theory landscape".
Fortschritte der Physik
.
59
(
3–
4):
243–
283.
arXiv
:
1009.5386
.
Bibcode
:
2011ForPh..59..243C
.
doi
:
10.1002/prop.201000093
.
S2CID
46634583
. |
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## Contents
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- [(Top)](https://en.wikipedia.org/wiki/String_theory_landscape)
- [1 Compactified Calabi–Yau manifolds](https://en.wikipedia.org/wiki/String_theory_landscape#Compactified_Calabi%E2%80%93Yau_manifolds)
- [2 Fine-tuning by the anthropic principle](https://en.wikipedia.org/wiki/String_theory_landscape#Fine-tuning_by_the_anthropic_principle)
Toggle Fine-tuning by the anthropic principle subsection
- [2\.1 Weinberg model](https://en.wikipedia.org/wiki/String_theory_landscape#Weinberg_model)
- [2\.2 Simplified approaches](https://en.wikipedia.org/wiki/String_theory_landscape#Simplified_approaches)
- [2\.3 Interpretation](https://en.wikipedia.org/wiki/String_theory_landscape#Interpretation)
- [2\.3.1 Cosmological constant problem](https://en.wikipedia.org/wiki/String_theory_landscape#Cosmological_constant_problem)
- [2\.4 Weak scale supersymmetry from the landscape](https://en.wikipedia.org/wiki/String_theory_landscape#Weak_scale_supersymmetry_from_the_landscape)
- [2\.4.1 Scientific relevance](https://en.wikipedia.org/wiki/String_theory_landscape#Scientific_relevance)
- [2\.4.2 Popular reception](https://en.wikipedia.org/wiki/String_theory_landscape#Popular_reception)
- [3 See also](https://en.wikipedia.org/wiki/String_theory_landscape#See_also)
- [4 References](https://en.wikipedia.org/wiki/String_theory_landscape#References)
- [5 External links](https://en.wikipedia.org/wiki/String_theory_landscape#External_links)
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# String theory landscape
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From Wikipedia, the free encyclopedia
Collection of possible string theory vacua
| [String theory](https://en.wikipedia.org/wiki/String_theory "String theory") |
|---|
| [](https://en.wikipedia.org/wiki/File:Calabi_yau_formatted.svg) |
| Fundamental objects |
| [String](https://en.wikipedia.org/wiki/String_\(physics\) "String (physics)") [Cosmic string](https://en.wikipedia.org/wiki/Cosmic_string "Cosmic string") [Brane](https://en.wikipedia.org/wiki/Brane "Brane") [D-brane](https://en.wikipedia.org/wiki/D-brane "D-brane") |
| Perturbative theory |
| [Bosonic](https://en.wikipedia.org/wiki/Bosonic_string_theory "Bosonic string theory") [Superstring](https://en.wikipedia.org/wiki/Superstring_theory "Superstring theory") ([Type I](https://en.wikipedia.org/wiki/Type_I_string_theory "Type I string theory"), [Type II](https://en.wikipedia.org/wiki/Type_II_string_theory "Type II string theory"), [Heterotic](https://en.wikipedia.org/wiki/Heterotic_string_theory "Heterotic string theory")) |
| Non-perturbative results |
| [S-duality](https://en.wikipedia.org/wiki/S-duality "S-duality") [T-duality](https://en.wikipedia.org/wiki/T-duality "T-duality") [U-duality](https://en.wikipedia.org/wiki/U-duality "U-duality") [M-theory](https://en.wikipedia.org/wiki/M-theory "M-theory") [F-theory](https://en.wikipedia.org/wiki/F-theory "F-theory") [AdS/CFT correspondence](https://en.wikipedia.org/wiki/AdS/CFT_correspondence "AdS/CFT correspondence") |
| Phenomenology |
| [Phenomenology](https://en.wikipedia.org/wiki/String_phenomenology "String phenomenology") [Cosmology](https://en.wikipedia.org/wiki/String_cosmology "String cosmology") [Brane cosmology](https://en.wikipedia.org/wiki/Brane_cosmology "Brane cosmology") [Landscape]() |
| Mathematics |
| [Geometric Langlands correspondence](https://en.wikipedia.org/wiki/Geometric_Langlands_correspondence "Geometric Langlands correspondence") [Mirror symmetry](https://en.wikipedia.org/wiki/Mirror_symmetry_\(string_theory\) "Mirror symmetry (string theory)") [Monstrous moonshine](https://en.wikipedia.org/wiki/Monstrous_moonshine "Monstrous moonshine") [Vertex algebra](https://en.wikipedia.org/wiki/Vertex_algebra "Vertex algebra") [K-theory](https://en.wikipedia.org/wiki/K-theory_\(physics\) "K-theory (physics)") |
| Related concepts [Theory of everything](https://en.wikipedia.org/wiki/Theory_of_everything "Theory of everything") [Conformal field theory](https://en.wikipedia.org/wiki/Conformal_field_theory "Conformal field theory") [Quantum gravity](https://en.wikipedia.org/wiki/Quantum_gravity "Quantum gravity") [Supersymmetry](https://en.wikipedia.org/wiki/Supersymmetry "Supersymmetry") [Supergravity](https://en.wikipedia.org/wiki/Supergravity "Supergravity") [Twistor string theory](https://en.wikipedia.org/wiki/Twistor_string_theory "Twistor string theory") [*N* = 4 supersymmetric Yang–Mills theory](https://en.wikipedia.org/wiki/N_%3D_4_supersymmetric_Yang%E2%80%93Mills_theory "N = 4 supersymmetric Yang–Mills theory") [Kaluza–Klein theory](https://en.wikipedia.org/wiki/Kaluza%E2%80%93Klein_theory "Kaluza–Klein theory") [Multiverse](https://en.wikipedia.org/wiki/Multiverse "Multiverse") [Holographic principle](https://en.wikipedia.org/wiki/Holographic_principle "Holographic principle") |
| Theorists [Aganagić](https://en.wikipedia.org/wiki/Mina_Aganagi%C4%87 "Mina Aganagić") [Arkani-Hamed](https://en.wikipedia.org/wiki/Nima_Arkani-Hamed "Nima Arkani-Hamed") [Atiyah](https://en.wikipedia.org/wiki/Michael_Atiyah "Michael Atiyah") [Banks](https://en.wikipedia.org/wiki/Tom_Banks_\(physicist\) "Tom Banks (physicist)") [Berenstein](https://en.wikipedia.org/wiki/David_Berenstein "David Berenstein") [Bousso](https://en.wikipedia.org/wiki/Raphael_Bousso "Raphael Bousso") [Costello](https://en.wikipedia.org/wiki/Kevin_Costello "Kevin Costello") [Curtright](https://en.wikipedia.org/wiki/Thomas_Curtright "Thomas Curtright") [Dijkgraaf](https://en.wikipedia.org/wiki/Robbert_Dijkgraaf "Robbert Dijkgraaf") [Distler](https://en.wikipedia.org/wiki/Jacques_Distler "Jacques Distler") [Douglas](https://en.wikipedia.org/wiki/Michael_R._Douglas "Michael R. Douglas") [Duff](https://en.wikipedia.org/wiki/Michael_Duff_\(physicist\) "Michael Duff (physicist)") [Dvali](https://en.wikipedia.org/wiki/Gia_Dvali "Gia Dvali") [Ferrara](https://en.wikipedia.org/wiki/Sergio_Ferrara "Sergio Ferrara") [Fischler](https://en.wikipedia.org/wiki/Willy_Fischler "Willy Fischler") [Friedan](https://en.wikipedia.org/wiki/Daniel_Friedan "Daniel Friedan") [Gates](https://en.wikipedia.org/wiki/Sylvester_James_Gates "Sylvester James Gates") [Gliozzi](https://en.wikipedia.org/wiki/Ferdinando_Gliozzi "Ferdinando Gliozzi") [Gopakumar](https://en.wikipedia.org/wiki/Rajesh_Gopakumar "Rajesh Gopakumar") [Green](https://en.wikipedia.org/wiki/Michael_Green_\(physicist\) "Michael Green (physicist)") [Greene](https://en.wikipedia.org/wiki/Brian_Greene "Brian Greene") [Gross](https://en.wikipedia.org/wiki/David_Gross "David Gross") [Gubser](https://en.wikipedia.org/wiki/Steven_Gubser "Steven Gubser") [Gukov](https://en.wikipedia.org/wiki/Sergei_Gukov "Sergei Gukov") [Guth](https://en.wikipedia.org/wiki/Alan_Guth "Alan Guth") [Hanson](https://en.wikipedia.org/wiki/Andrew_J._Hanson "Andrew J. Hanson") [Harvey](https://en.wikipedia.org/wiki/Jeffrey_A._Harvey "Jeffrey A. Harvey") [Hořava](https://en.wikipedia.org/wiki/Petr_Ho%C5%99ava_\(theorist\) "Petr Hořava (theorist)") [Horowitz](https://en.wikipedia.org/wiki/Gary_Horowitz "Gary Horowitz") [Gibbons](https://en.wikipedia.org/wiki/Gary_Gibbons "Gary Gibbons") [Kachru](https://en.wikipedia.org/wiki/Shamit_Kachru "Shamit Kachru") [Kaku](https://en.wikipedia.org/wiki/Michio_Kaku "Michio Kaku") [Kallosh](https://en.wikipedia.org/wiki/Renata_Kallosh "Renata Kallosh") [Kaluza](https://en.wikipedia.org/wiki/Theodor_Kaluza "Theodor Kaluza") [Kapustin](https://en.wikipedia.org/wiki/Anton_Kapustin "Anton Kapustin") [Klebanov](https://en.wikipedia.org/wiki/Igor_Klebanov "Igor Klebanov") [Knizhnik](https://en.wikipedia.org/wiki/Vadim_Knizhnik "Vadim Knizhnik") [Kontsevich](https://en.wikipedia.org/wiki/Maxim_Kontsevich "Maxim Kontsevich") [Klein](https://en.wikipedia.org/wiki/Oskar_Klein "Oskar Klein") [Linde](https://en.wikipedia.org/wiki/Andrei_Linde "Andrei Linde") [Maldacena](https://en.wikipedia.org/wiki/Juan_Mart%C3%ADn_Maldacena "Juan Martín Maldacena") [Mandelstam](https://en.wikipedia.org/wiki/Stanley_Mandelstam "Stanley Mandelstam") [Marolf](https://en.wikipedia.org/wiki/Donald_Marolf "Donald Marolf") [Martinec](https://en.wikipedia.org/wiki/Emil_Martinec "Emil Martinec") [Minwalla](https://en.wikipedia.org/wiki/Shiraz_Minwalla "Shiraz Minwalla") [Moore](https://en.wikipedia.org/wiki/Greg_Moore_\(physicist\) "Greg Moore (physicist)") [Motl](https://en.wikipedia.org/wiki/Lubo%C5%A1_Motl "Luboš Motl") [Mukhi](https://en.wikipedia.org/wiki/Sunil_Mukhi "Sunil Mukhi") [Myers](https://en.wikipedia.org/wiki/Robert_Myers_\(physicist\) "Robert Myers (physicist)") [Nanopoulos](https://en.wikipedia.org/wiki/Dimitri_Nanopoulos "Dimitri Nanopoulos") [Năstase](https://en.wikipedia.org/wiki/Hora%C8%9Biu_N%C4%83stase "Horațiu Năstase") [Nekrasov](https://en.wikipedia.org/wiki/Nikita_Nekrasov "Nikita Nekrasov") [Neveu](https://en.wikipedia.org/wiki/Andr%C3%A9_Neveu "André Neveu") [Nielsen](https://en.wikipedia.org/wiki/Holger_Bech_Nielsen "Holger Bech Nielsen") [van Nieuwenhuizen](https://en.wikipedia.org/wiki/Peter_van_Nieuwenhuizen "Peter van Nieuwenhuizen") [Novikov](https://en.wikipedia.org/wiki/Sergei_Novikov_\(mathematician\) "Sergei Novikov (mathematician)") [Olive](https://en.wikipedia.org/wiki/David_Olive "David Olive") [Ooguri](https://en.wikipedia.org/wiki/Hirosi_Ooguri "Hirosi Ooguri") [Ovrut](https://en.wikipedia.org/wiki/Burt_Ovrut "Burt Ovrut") [Polchinski](https://en.wikipedia.org/wiki/Joseph_Polchinski "Joseph Polchinski") [Polyakov](https://en.wikipedia.org/wiki/Alexander_Markovich_Polyakov "Alexander Markovich Polyakov") [Rajaraman](https://en.wikipedia.org/wiki/Arvind_Rajaraman "Arvind Rajaraman") [Ramond](https://en.wikipedia.org/wiki/Pierre_Ramond "Pierre Ramond") [Randall](https://en.wikipedia.org/wiki/Lisa_Randall "Lisa Randall") [Randjbar-Daemi](https://en.wikipedia.org/wiki/Seifallah_Randjbar-Daemi "Seifallah Randjbar-Daemi") [Roček](https://en.wikipedia.org/wiki/Martin_Ro%C4%8Dek "Martin Roček") [Rohm](https://en.wikipedia.org/wiki/Ryan_Rohm "Ryan Rohm") [Sagnotti](https://en.wikipedia.org/wiki/Augusto_Sagnotti "Augusto Sagnotti") [Scherk](https://en.wikipedia.org/wiki/Jo%C3%ABl_Scherk "Joël Scherk") [Schwarz](https://en.wikipedia.org/wiki/John_Henry_Schwarz "John Henry Schwarz") [Seiberg](https://en.wikipedia.org/wiki/Nathan_Seiberg "Nathan Seiberg") [Sen](https://en.wikipedia.org/wiki/Ashoke_Sen "Ashoke Sen") [Shenker](https://en.wikipedia.org/wiki/Stephen_Shenker "Stephen Shenker") [Siegel](https://en.wikipedia.org/wiki/Warren_Siegel "Warren Siegel") [Silverstein](https://en.wikipedia.org/wiki/Eva_Silverstein "Eva Silverstein") [Sơn](https://en.wikipedia.org/wiki/%C4%90%C3%A0m_Thanh_S%C6%A1n "Đàm Thanh Sơn") [Staudacher](https://en.wikipedia.org/wiki/Matthias_Staudacher "Matthias Staudacher") [Steinhardt](https://en.wikipedia.org/wiki/Paul_Steinhardt "Paul Steinhardt") [Strominger](https://en.wikipedia.org/wiki/Andrew_Strominger "Andrew Strominger") [Sundrum](https://en.wikipedia.org/wiki/Raman_Sundrum "Raman Sundrum") [Susskind](https://en.wikipedia.org/wiki/Leonard_Susskind "Leonard Susskind") ['t Hooft](https://en.wikipedia.org/wiki/Gerard_%27t_Hooft "Gerard 't Hooft") [Townsend](https://en.wikipedia.org/wiki/Paul_Townsend "Paul Townsend") [Trivedi](https://en.wikipedia.org/wiki/Sandip_Trivedi "Sandip Trivedi") [Turok](https://en.wikipedia.org/wiki/Neil_Turok "Neil Turok") [Vafa](https://en.wikipedia.org/wiki/Cumrun_Vafa "Cumrun Vafa") [Veneziano](https://en.wikipedia.org/wiki/Gabriele_Veneziano "Gabriele Veneziano") [Verlinde](https://en.wikipedia.org/wiki/Erik_Verlinde "Erik Verlinde") [Verlinde](https://en.wikipedia.org/wiki/Herman_Verlinde "Herman Verlinde") [Wess](https://en.wikipedia.org/wiki/Julius_Wess "Julius Wess") [Witten](https://en.wikipedia.org/wiki/Edward_Witten "Edward Witten") [Yau](https://en.wikipedia.org/wiki/Shing-Tung_Yau "Shing-Tung Yau") [Yoneya](https://en.wikipedia.org/wiki/Tamiaki_Yoneya "Tamiaki Yoneya") [Zamolodchikov](https://en.wikipedia.org/wiki/Alexander_Zamolodchikov "Alexander Zamolodchikov") [Zamolodchikov](https://en.wikipedia.org/wiki/Alexei_Zamolodchikov "Alexei Zamolodchikov") [Zaslow](https://en.wikipedia.org/wiki/Eric_Zaslow "Eric Zaslow") [Zumino](https://en.wikipedia.org/wiki/Bruno_Zumino "Bruno Zumino") [Zwiebach](https://en.wikipedia.org/wiki/Barton_Zwiebach "Barton Zwiebach") |
| [History](https://en.wikipedia.org/wiki/History_of_string_theory "History of string theory") [Glossary](https://en.wikipedia.org/wiki/Glossary_of_string_theory "Glossary of string theory") |
| [v](https://en.wikipedia.org/wiki/Template:String_theory "Template:String theory") [t](https://en.wikipedia.org/wiki/Template_talk:String_theory "Template talk:String theory") [e](https://en.wikipedia.org/wiki/Special:EditPage/Template:String_theory "Special:EditPage/Template:String theory") |
In [string theory](https://en.wikipedia.org/wiki/String_theory "String theory"), the **string theory landscape** (or **landscape of vacua**) is the collection of possible [false vacua](https://en.wikipedia.org/wiki/False_vacuum "False vacuum"),[\[1\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-Ashok-1) together comprising a collective "landscape" of choices of parameters governing [compactifications](https://en.wikipedia.org/wiki/Compactification_\(physics\) "Compactification (physics)").
The term "landscape" comes from the notion of a [fitness landscape](https://en.wikipedia.org/wiki/Fitness_landscape "Fitness landscape") in [evolutionary biology](https://en.wikipedia.org/wiki/Evolutionary_biology "Evolutionary biology").[\[2\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-2) It was first applied to cosmology by [Lee Smolin](https://en.wikipedia.org/wiki/Lee_Smolin "Lee Smolin") in his book *[The Life of the Cosmos](https://en.wikipedia.org/wiki/The_Life_of_the_Cosmos "The Life of the Cosmos")* (1997), and was first used in the context of string theory by [Leonard Susskind](https://en.wikipedia.org/wiki/Leonard_Susskind "Leonard Susskind").[\[3\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-3)
## Compactified Calabi–Yau manifolds
\[[edit](https://en.wikipedia.org/w/index.php?title=String_theory_landscape&action=edit§ion=1 "Edit section: Compactified Calabi–Yau manifolds")\]
Main article: [Compactification (physics)](https://en.wikipedia.org/wiki/Compactification_\(physics\) "Compactification (physics)")
In string theory, the estimated count of distinct flux vacua is commonly stated as having a lower bound of 10 500 {\\displaystyle 10^{500}} ,[\[4\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-4) but more recently this has been revised to 10 272 , 000 {\\displaystyle 10^{272,000}} ,[\[5\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-5) and the true number may still be far higher. The large number of possibilities arises from choices of [Calabi–Yau manifolds](https://en.wikipedia.org/wiki/Calabi%E2%80%93Yau_manifold "Calabi–Yau manifold") and choices of generalized [magnetic fluxes](https://en.wikipedia.org/wiki/Magnetic_flux "Magnetic flux") over various [homology](https://en.wikipedia.org/wiki/Homology_\(mathematics\) "Homology (mathematics)") cycles, found in [F-theory](https://en.wikipedia.org/wiki/F-theory "F-theory").
If there is no structure in the space of vacua, the problem of finding one with a sufficiently small cosmological constant is [NP complete](https://en.wikipedia.org/wiki/NP_complete "NP complete").[\[6\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-6) This is a version of the [subset sum problem](https://en.wikipedia.org/wiki/Subset_sum_problem "Subset sum problem").
A possible mechanism of string theory vacuum stabilization, now known as the **KKLT mechanism**, was proposed in 2003 by [Shamit Kachru](https://en.wikipedia.org/wiki/Shamit_Kachru "Shamit Kachru"), [Renata Kallosh](https://en.wikipedia.org/wiki/Renata_Kallosh "Renata Kallosh"), [Andrei Linde](https://en.wikipedia.org/wiki/Andrei_Linde "Andrei Linde"), and [Sandip Trivedi](https://en.wikipedia.org/wiki/Sandip_Trivedi "Sandip Trivedi").[\[7\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-7)
## Fine-tuning by the anthropic principle
\[[edit](https://en.wikipedia.org/w/index.php?title=String_theory_landscape&action=edit§ion=2 "Edit section: Fine-tuning by the anthropic principle")\]
Main articles: [Fine-tuning (physics)](https://en.wikipedia.org/wiki/Fine-tuning_\(physics\) "Fine-tuning (physics)") and [Anthropic principle](https://en.wikipedia.org/wiki/Anthropic_principle "Anthropic principle")
[Fine-tuning](https://en.wikipedia.org/wiki/Fine-tuning_\(physics\) "Fine-tuning (physics)") of constants like the [cosmological constant](https://en.wikipedia.org/wiki/Cosmological_constant "Cosmological constant") or the [Higgs boson](https://en.wikipedia.org/wiki/Higgs_boson "Higgs boson") mass is usually assumed to occur for precise physical reasons as opposed to taking their particular values at random. That is, these values should be uniquely consistent with underlying physical laws.
The number of theoretically allowed configurations has prompted suggestions\[*[according to whom?](https://en.wikipedia.org/wiki/Wikipedia:Manual_of_Style/Words_to_watch#Unsupported_attributions "Wikipedia:Manual of Style/Words to watch")*\] that this is not the case, and that many different vacua are physically realized.[\[8\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-8) The [anthropic principle](https://en.wikipedia.org/wiki/Anthropic_principle "Anthropic principle") proposes that fundamental constants may have the values they have because such values are necessary for life (and therefore intelligent observers to measure the constants). The *anthropic landscape* thus refers to the collection of those portions of the landscape that are suitable for supporting intelligent life.
### Weinberg model
\[[edit](https://en.wikipedia.org/w/index.php?title=String_theory_landscape&action=edit§ion=3 "Edit section: Weinberg model")\]
In 1987, [Steven Weinberg](https://en.wikipedia.org/wiki/Steven_Weinberg "Steven Weinberg") proposed that the observed value of the [cosmological constant](https://en.wikipedia.org/wiki/Cosmological_constant "Cosmological constant") was so small because it is impossible for life to occur in a universe with a much larger cosmological constant.[\[9\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-9)
Weinberg attempted to predict the magnitude of the cosmological constant based on probabilistic arguments. Other attempts\[*[which?](https://en.wikipedia.org/wiki/Wikipedia:Avoid_weasel_words "Wikipedia:Avoid weasel words")*\] have been made to apply similar reasoning to models of particle physics.[\[10\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-10)
Such attempts are based in the general ideas of [Bayesian probability](https://en.wikipedia.org/wiki/Bayesian_probability "Bayesian probability"); interpreting probability in a context where it is only possible to draw one [sample](https://en.wikipedia.org/wiki/Sample_size "Sample size") from a [distribution](https://en.wikipedia.org/wiki/Probability_distribution "Probability distribution") is problematic in [frequentist probability](https://en.wikipedia.org/wiki/Frequentist_probability "Frequentist probability") but not in Bayesian probability, which is not defined in terms of the frequency of repeated events.
In such a framework, the probability P ( x ) {\\displaystyle P(x)}  of observing some fundamental parameters x {\\displaystyle x}  is given by,
P
(
x
)
\=
P
p
r
i
o
r
(
x
)
×
P
s
e
l
e
c
t
i
o
n
(
x
)
,
{\\displaystyle P(x)=P\_{\\mathrm {prior} }(x)\\times P\_{\\mathrm {selection} }(x),}

where P p r i o r {\\displaystyle P\_{\\mathrm {prior} }}  is the prior probability, from fundamental theory, of the parameters x {\\displaystyle x}  and P s e l e c t i o n {\\displaystyle P\_{\\mathrm {selection} }}  is the "anthropic selection function", determined by the number of "observers" that would occur in the universe with parameters x {\\displaystyle x} .\[*[citation needed](https://en.wikipedia.org/wiki/Wikipedia:Citation_needed "Wikipedia:Citation needed")*\]
These probabilistic arguments are the most controversial aspect of the landscape. Technical criticisms of these proposals have pointed out that:\[*[citation needed](https://en.wikipedia.org/wiki/Wikipedia:Citation_needed "Wikipedia:Citation needed")*\]\[*[year needed](https://en.wikipedia.org/wiki/Wikipedia:Manual_of_Style/Dates_and_numbers "Wikipedia:Manual of Style/Dates and numbers")*\]
- The function
P
p
r
i
o
r
{\\displaystyle P\_{\\mathrm {prior} }}

is completely unknown in string theory and may be impossible to define or interpret in any sensible probabilistic way.
- The function
P
s
e
l
e
c
t
i
o
n
{\\displaystyle P\_{\\mathrm {selection} }}

is completely unknown, since so little is known about the origin of life. Simplified criteria (such as the number of galaxies) must be used as a proxy for the number of observers. Moreover, it may never be possible to compute it for parameters radically different from those of the observable universe.
### Simplified approaches
\[[edit](https://en.wikipedia.org/w/index.php?title=String_theory_landscape&action=edit§ion=4 "Edit section: Simplified approaches")\]
[Tegmark](https://en.wikipedia.org/wiki/Max_Tegmark "Max Tegmark") *et al.* have recently considered these objections and proposed a simplified anthropic scenario for [axion](https://en.wikipedia.org/wiki/Axion "Axion") [dark matter](https://en.wikipedia.org/wiki/Dark_matter "Dark matter") in which they argue that the first two of these problems do not apply.[\[11\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-11)
Vilenkin and collaborators have proposed a consistent way to define the probabilities for a given vacuum.[\[12\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-12)
A problem with many of the simplified approaches people\[*[who?](https://en.wikipedia.org/wiki/Wikipedia:Manual_of_Style/Words_to_watch#Unsupported_attributions "Wikipedia:Manual of Style/Words to watch")*\] have tried is that they "predict" a cosmological constant that is too large by a factor of 10–1000 orders of magnitude (depending on one's assumptions) and hence suggest that the cosmic acceleration should be much more rapid than is observed.[\[13\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-13)[\[14\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-14)[\[15\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-15)
### Interpretation
\[[edit](https://en.wikipedia.org/w/index.php?title=String_theory_landscape&action=edit§ion=5 "Edit section: Interpretation")\]
Few dispute the large number of metastable vacua.\[*[citation needed](https://en.wikipedia.org/wiki/Wikipedia:Citation_needed "Wikipedia:Citation needed")*\] The existence, meaning, and scientific relevance of the anthropic landscape, however, remain controversial.\[*[further explanation needed](https://en.wikipedia.org/wiki/Wikipedia:Please_clarify "Wikipedia:Please clarify")*\]
#### Cosmological constant problem
\[[edit](https://en.wikipedia.org/w/index.php?title=String_theory_landscape&action=edit§ion=6 "Edit section: Cosmological constant problem")\]
[Andrei Linde](https://en.wikipedia.org/wiki/Andrei_Linde "Andrei Linde"), [Sir Martin Rees](https://en.wikipedia.org/wiki/Sir_Martin_Rees "Sir Martin Rees") and [Leonard Susskind](https://en.wikipedia.org/wiki/Leonard_Susskind "Leonard Susskind") advocate it as a solution to the [cosmological constant problem](https://en.wikipedia.org/wiki/Cosmological_constant_problem "Cosmological constant problem").\[*[citation needed](https://en.wikipedia.org/wiki/Wikipedia:Citation_needed "Wikipedia:Citation needed")*\]
### Weak scale supersymmetry from the landscape
\[[edit](https://en.wikipedia.org/w/index.php?title=String_theory_landscape&action=edit§ion=7 "Edit section: Weak scale supersymmetry from the landscape")\]
The string landscape ideas can be applied to the notion of weak scale supersymmetry and the Little Hierarchy problem. For string vacua which include the MSSM (Minimal Supersymmetric Standard Model) as the low energy effective field theory, all values of SUSY breaking fields are expected to be equally likely on the landscape. This led Douglas[\[16\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-16) and others to propose that the SUSY breaking scale is distributed as a power law in the landscape P p r i o r ∼ m s o f t 2 n F \+ n D − 1 {\\displaystyle P\_{prior}\\sim m\_{soft}^{2n\_{F}+n\_{D}-1}}  where n F {\\displaystyle n\_{F}}  is the number of F-breaking fields (distributed as complex numbers) and n D {\\displaystyle n\_{D}}  is the number of D-breaking fields (distributed as real numbers). Next, one may impose the Agrawal, Barr, Donoghue, Seckel (ABDS) anthropic requirement[\[17\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-17) that the derived weak scale lie within a factor of a few of our measured value (lest nuclei as needed for life as we know it become unstable (the atomic principle)). Combining these effects with a mild power-law draw to large soft SUSY breaking terms, one may calculate the Higgs boson and superparticle masses expected from the landscape.[\[18\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-18) The Higgs mass probability distribution peaks around 125 GeV while sparticles (with the exception of light higgsinos) tend to lie well beyond current LHC search limits. This approach is an example of the application of stringy naturalness.
#### Scientific relevance
\[[edit](https://en.wikipedia.org/w/index.php?title=String_theory_landscape&action=edit§ion=8 "Edit section: Scientific relevance")\]
[David Gross](https://en.wikipedia.org/wiki/David_Gross "David Gross") suggests\[*[citation needed](https://en.wikipedia.org/wiki/Wikipedia:Citation_needed "Wikipedia:Citation needed")*\] that the idea is inherently unscientific, unfalsifiable or premature. A famous debate on the anthropic landscape of string theory is the [Smolin–Susskind debate](https://en.wikipedia.org/wiki/Smolin%E2%80%93Susskind_debate "Smolin–Susskind debate") on the merits of the landscape.
#### Popular reception
\[[edit](https://en.wikipedia.org/w/index.php?title=String_theory_landscape&action=edit§ion=9 "Edit section: Popular reception")\]
There are several popular books about the anthropic principle in cosmology.[\[19\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-19) The authors of two physics blogs, [Lubos Motl](https://en.wikipedia.org/wiki/Lubos_Motl "Lubos Motl") and [Peter Woit](https://en.wikipedia.org/wiki/Peter_Woit "Peter Woit"), are opposed to this use of the anthropic principle.\[*[why?](https://en.wikipedia.org/wiki/Wikipedia:Please_clarify "Wikipedia:Please clarify")*\][\[20\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-20)
## See also
\[[edit](https://en.wikipedia.org/w/index.php?title=String_theory_landscape&action=edit§ion=10 "Edit section: See also")\]
- [](https://en.wikipedia.org/wiki/File:Stylised_atom_with_three_Bohr_model_orbits_and_stylised_nucleus.svg)[Physics portal](https://en.wikipedia.org/wiki/Portal:Physics "Portal:Physics")
- [Swampland](https://en.wikipedia.org/wiki/Swampland_\(physics\) "Swampland (physics)")
- [Extra dimensions](https://en.wikipedia.org/wiki/String_theory#Extra_dimensions "String theory")
- [M-theory](https://en.wikipedia.org/wiki/M-theory "M-theory")
## References
\[[edit](https://en.wikipedia.org/w/index.php?title=String_theory_landscape&action=edit§ion=11 "Edit section: References")\]
1. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-Ashok_1-0)** The number of metastable vacua is not known exactly, but commonly quoted estimates are of the order 10500. See [M. Douglas](https://en.wikipedia.org/wiki/Michael_R._Douglas "Michael R. Douglas"), "The statistics of string / M theory vacua", *JHEP* **0305**, 46 (2003). [arXiv](https://en.wikipedia.org/wiki/ArXiv_\(identifier\) "ArXiv (identifier)"):[hep-th/0303194](https://arxiv.org/abs/hep-th/0303194); S. Ashok and M. Douglas, "Counting flux vacua", *JHEP* **0401**, 060 (2004).
2. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-2)**
Baggott, Jim (2018). [*Quantum Space Loop Quantum Gravity and the Search for the Structure of Space, Time, and the Universe*](https://books.google.com/books?id=HwN6DwAAQBAJ&pg=PA288). Oxford University Press. p. 288. [ISBN](https://en.wikipedia.org/wiki/ISBN_\(identifier\) "ISBN (identifier)")
[978-0-19-253681-5](https://en.wikipedia.org/wiki/Special:BookSources/978-0-19-253681-5 "Special:BookSources/978-0-19-253681-5")
.
3. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-3)** L. Smolin, "Did the universe evolve?", *Classical and Quantum Gravity* **9**, 173–191 (1992). L. Smolin, *[The Life of the Cosmos](https://en.wikipedia.org/wiki/The_Life_of_the_Cosmos "The Life of the Cosmos")* (Oxford, 1997)
4. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-4)**
Read, James; Le Bihan, Baptiste (2021). ["The landscape and the multiverse: What's the problem?"](https://doi.org/10.1007%2Fs11229-021-03137-0). *Synthese*. **199** (3–4\): 7749–7771\. [doi](https://en.wikipedia.org/wiki/Doi_\(identifier\) "Doi (identifier)"):[10\.1007/s11229-021-03137-0](https://doi.org/10.1007%2Fs11229-021-03137-0). [S2CID](https://en.wikipedia.org/wiki/S2CID_\(identifier\) "S2CID (identifier)") [234815857](https://api.semanticscholar.org/CorpusID:234815857).
5. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-5)**
Taylor, Washington; Wang, Yi-Nan (2015). "The F-theory geometry with most flux vacua". *Journal of High Energy Physics*. **2015** (12): 164. [arXiv](https://en.wikipedia.org/wiki/ArXiv_\(identifier\) "ArXiv (identifier)"):[1511\.03209](https://arxiv.org/abs/1511.03209). [Bibcode](https://en.wikipedia.org/wiki/Bibcode_\(identifier\) "Bibcode (identifier)"):[2015JHEP...12..164T](https://ui.adsabs.harvard.edu/abs/2015JHEP...12..164T). [doi](https://en.wikipedia.org/wiki/Doi_\(identifier\) "Doi (identifier)"):[10\.1007/JHEP12(2015)164](https://doi.org/10.1007%2FJHEP12%282015%29164). [S2CID](https://en.wikipedia.org/wiki/S2CID_\(identifier\) "S2CID (identifier)") [41149049](https://api.semanticscholar.org/CorpusID:41149049).
6. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-6)**
Frederik Denef; Douglas, Michael R. (2007). "Computational complexity of the landscape". *Annals of Physics*. **322** (5): 1096–1142\. [arXiv](https://en.wikipedia.org/wiki/ArXiv_\(identifier\) "ArXiv (identifier)"):[hep-th/0602072](https://arxiv.org/abs/hep-th/0602072). [Bibcode](https://en.wikipedia.org/wiki/Bibcode_\(identifier\) "Bibcode (identifier)"):[2007AnPhy.322.1096D](https://ui.adsabs.harvard.edu/abs/2007AnPhy.322.1096D). [doi](https://en.wikipedia.org/wiki/Doi_\(identifier\) "Doi (identifier)"):[10\.1016/j.aop.2006.07.013](https://doi.org/10.1016%2Fj.aop.2006.07.013). [S2CID](https://en.wikipedia.org/wiki/S2CID_\(identifier\) "S2CID (identifier)") [281586](https://api.semanticscholar.org/CorpusID:281586).
7. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-7)**
Kachru, Shamit; Kallosh, Renata; Linde, Andrei; Trivedi, Sandip P. (2003). "de Sitter Vacua in String Theory". *Physical Review D*. **68** (4) 046005. [arXiv](https://en.wikipedia.org/wiki/ArXiv_\(identifier\) "ArXiv (identifier)"):[hep-th/0301240](https://arxiv.org/abs/hep-th/0301240). [Bibcode](https://en.wikipedia.org/wiki/Bibcode_\(identifier\) "Bibcode (identifier)"):[2003PhRvD..68d6005K](https://ui.adsabs.harvard.edu/abs/2003PhRvD..68d6005K). [doi](https://en.wikipedia.org/wiki/Doi_\(identifier\) "Doi (identifier)"):[10\.1103/PhysRevD.68.046005](https://doi.org/10.1103%2FPhysRevD.68.046005). [S2CID](https://en.wikipedia.org/wiki/S2CID_\(identifier\) "S2CID (identifier)") [119482182](https://api.semanticscholar.org/CorpusID:119482182).
8. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-8)**
L. Susskind, "The anthropic landscape of string theory",
[arXiv](https://en.wikipedia.org/wiki/ArXiv_\(identifier\) "ArXiv (identifier)"):[hep-th/0302219](https://arxiv.org/abs/hep-th/0302219).
9. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-9)** S. Weinberg, "Anthropic bound on the cosmological constant", *Phys. Rev. Lett.* **59**, 2607 (1987).
10. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-10)**
S. M. Carroll, "Is our universe natural?" (2005)
[arXiv](https://en.wikipedia.org/wiki/ArXiv_\(identifier\) "ArXiv (identifier)"):[hep-th/0512148](https://arxiv.org/abs/hep-th/0512148) reviews a number of proposals in preprints dated 2004/5.
11. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-11)**
M. Tegmark, A. Aguirre, M. Rees and F. Wilczek, "Dimensionless constants, cosmology and other dark matters",
[arXiv](https://en.wikipedia.org/wiki/ArXiv_\(identifier\) "ArXiv (identifier)"):[astro-ph/0511774](https://arxiv.org/abs/astro-ph/0511774). F. Wilczek, "Enlightenment, knowledge, ignorance, temptation",
[arXiv](https://en.wikipedia.org/wiki/ArXiv_\(identifier\) "ArXiv (identifier)"):[hep-ph/0512187](https://arxiv.org/abs/hep-ph/0512187). See also the discussion at [\[1\]](http://www.math.columbia.edu/~woit/wordpress/?p=310).
12. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-12)**
See, *e.g.*
Alexander Vilenkin (2007). "A measure of the multiverse". *Journal of Physics A: Mathematical and Theoretical*. **40** (25): 6777–6785\. [arXiv](https://en.wikipedia.org/wiki/ArXiv_\(identifier\) "ArXiv (identifier)"):[hep-th/0609193](https://arxiv.org/abs/hep-th/0609193). [Bibcode](https://en.wikipedia.org/wiki/Bibcode_\(identifier\) "Bibcode (identifier)"):[2007JPhA...40.6777V](https://ui.adsabs.harvard.edu/abs/2007JPhA...40.6777V). [doi](https://en.wikipedia.org/wiki/Doi_\(identifier\) "Doi (identifier)"):[10\.1088/1751-8113/40/25/S22](https://doi.org/10.1088%2F1751-8113%2F40%2F25%2FS22). [S2CID](https://en.wikipedia.org/wiki/S2CID_\(identifier\) "S2CID (identifier)") [119390736](https://api.semanticscholar.org/CorpusID:119390736).
13. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-13)**
Abraham Loeb (2006). "An observational test for the anthropic origin of the cosmological constant". *Journal of Cosmology and Astroparticle Physics*. **0605** (5): 009. [arXiv](https://en.wikipedia.org/wiki/ArXiv_\(identifier\) "ArXiv (identifier)"):[astro-ph/0604242](https://arxiv.org/abs/astro-ph/0604242). [Bibcode](https://en.wikipedia.org/wiki/Bibcode_\(identifier\) "Bibcode (identifier)"):[2006JCAP...05..009L](https://ui.adsabs.harvard.edu/abs/2006JCAP...05..009L). [doi](https://en.wikipedia.org/wiki/Doi_\(identifier\) "Doi (identifier)"):[10\.1088/1475-7516/2006/05/009](https://doi.org/10.1088%2F1475-7516%2F2006%2F05%2F009). [S2CID](https://en.wikipedia.org/wiki/S2CID_\(identifier\) "S2CID (identifier)") [39340203](https://api.semanticscholar.org/CorpusID:39340203).
14. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-14)**
Jaume Garriga & Alexander Vilenkin (2006). "Anthropic prediction for Lambda and the Q catastrophe". *Prog. Theor. Phys. Suppl*. **163**: 245–57\. [arXiv](https://en.wikipedia.org/wiki/ArXiv_\(identifier\) "ArXiv (identifier)"):[hep-th/0508005](https://arxiv.org/abs/hep-th/0508005). [Bibcode](https://en.wikipedia.org/wiki/Bibcode_\(identifier\) "Bibcode (identifier)"):[2006PThPS.163..245G](https://ui.adsabs.harvard.edu/abs/2006PThPS.163..245G). [doi](https://en.wikipedia.org/wiki/Doi_\(identifier\) "Doi (identifier)"):[10\.1143/PTPS.163.245](https://doi.org/10.1143%2FPTPS.163.245). [S2CID](https://en.wikipedia.org/wiki/S2CID_\(identifier\) "S2CID (identifier)") [118936307](https://api.semanticscholar.org/CorpusID:118936307).
15. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-15)**
Delia Schwartz-Perlov & Alexander Vilenkin (2006). "Probabilities in the Bousso-Polchinski multiverse". *Journal of Cosmology and Astroparticle Physics*. **0606** (6): 010. [arXiv](https://en.wikipedia.org/wiki/ArXiv_\(identifier\) "ArXiv (identifier)"):[hep-th/0601162](https://arxiv.org/abs/hep-th/0601162). [Bibcode](https://en.wikipedia.org/wiki/Bibcode_\(identifier\) "Bibcode (identifier)"):[2006JCAP...06..010S](https://ui.adsabs.harvard.edu/abs/2006JCAP...06..010S). [doi](https://en.wikipedia.org/wiki/Doi_\(identifier\) "Doi (identifier)"):[10\.1088/1475-7516/2006/06/010](https://doi.org/10.1088%2F1475-7516%2F2006%2F06%2F010). [S2CID](https://en.wikipedia.org/wiki/S2CID_\(identifier\) "S2CID (identifier)") [119337679](https://api.semanticscholar.org/CorpusID:119337679).
16. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-16)**
M. R. Douglas, "Statistical analysis of the supersymmetry breaking scale",
[arXiv](https://en.wikipedia.org/wiki/ArXiv_\(identifier\) "ArXiv (identifier)"):[hep-th/0405279](https://arxiv.org/abs/hep-th/0405279).
17. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-17)**
V. Agrawal, S. M. Barr, J. F. Donoghue and D. Seckel, "Anthropic considerations in multiple domain theories and the scale of electroweak symmetry breaking", *Phys. Rev. Lett.* **80**, 1822 (1998).
[arXiv](https://en.wikipedia.org/wiki/ArXiv_\(identifier\) "ArXiv (identifier)"):[hep-ph/9801253](https://arxiv.org/abs/hep-ph/9801253)
18. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-18)**
H. Baer, V. Barger, H. Serce and K. Sinha, "Higgs and superparticle mass predictions from the landscape", *JHEP* **03**, 002 (2018),
[arXiv](https://en.wikipedia.org/wiki/ArXiv_\(identifier\) "ArXiv (identifier)"):[1712\.01399](https://arxiv.org/abs/1712.01399) .
19. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-19)** L. Susskind, *The cosmic landscape: string theory and the illusion of intelligent design* (Little, Brown, 2005). M. J. Rees, *Just six numbers: the deep forces that shape the universe* (Basic Books, 2001). R. Bousso and J. Polchinski, "The string theory landscape", *Sci. Am.* **291**, 60–69 (2004).
20. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-20)** Motl's blog criticized the anthropic principle and Woit's [blog](http://www.math.columbia.edu/~woit/blog/) frequently attacks the anthropic string landscape.
## External links
\[[edit](https://en.wikipedia.org/w/index.php?title=String_theory_landscape&action=edit§ion=12 "Edit section: External links")\]
- [String landscape; moduli stabilization; flux vacua; flux compactification](http://xstructure.inr.ac.ru/x-bin/theme2.py?arxiv=hep-th&level=1&index1=5460697) on [arxiv.org](https://en.wikipedia.org/wiki/Arxiv.org "Arxiv.org").
- [Cvetič, Mirjam](https://en.wikipedia.org/wiki/Mirjam_Cveti%C4%8D "Mirjam Cvetič"); García-Etxebarria, Iñaki; Halverson, James (March 2011). "On the computation of non-perturbative effective potentials in the string theory landscape". *Fortschritte der Physik*. **59** (3–4\): 243–283\. [arXiv](https://en.wikipedia.org/wiki/ArXiv_\(identifier\) "ArXiv (identifier)"):[1009\.5386](https://arxiv.org/abs/1009.5386). [Bibcode](https://en.wikipedia.org/wiki/Bibcode_\(identifier\) "Bibcode (identifier)"):[2011ForPh..59..243C](https://ui.adsabs.harvard.edu/abs/2011ForPh..59..243C). [doi](https://en.wikipedia.org/wiki/Doi_\(identifier\) "Doi (identifier)"):[10\.1002/prop.201000093](https://doi.org/10.1002%2Fprop.201000093). [S2CID](https://en.wikipedia.org/wiki/S2CID_\(identifier\) "S2CID (identifier)") [46634583](https://api.semanticscholar.org/CorpusID:46634583).
| [v](https://en.wikipedia.org/wiki/Template:String_theory_topics "Template:String theory topics") [t](https://en.wikipedia.org/wiki/Template_talk:String_theory_topics "Template talk:String theory topics") [e](https://en.wikipedia.org/wiki/Special:EditPage/Template:String_theory_topics "Special:EditPage/Template:String theory topics")[String theory](https://en.wikipedia.org/wiki/String_theory "String theory") | |
|---|---|
| Background | [Strings](https://en.wikipedia.org/wiki/String_\(physics\) "String (physics)") [Cosmic strings](https://en.wikipedia.org/wiki/Cosmic_string "Cosmic string") [History of string theory](https://en.wikipedia.org/wiki/History_of_string_theory "History of string theory") [First superstring revolution](https://en.wikipedia.org/wiki/First_superstring_revolution "First superstring revolution") [Second superstring revolution](https://en.wikipedia.org/wiki/Second_superstring_revolution "Second superstring revolution") [String theory landscape]() |
| Theory | [Nambu–Goto action](https://en.wikipedia.org/wiki/Nambu%E2%80%93Goto_action "Nambu–Goto action") [Polyakov action](https://en.wikipedia.org/wiki/Polyakov_action "Polyakov action") [Bosonic string theory](https://en.wikipedia.org/wiki/Bosonic_string_theory "Bosonic string theory") [Superstring theory](https://en.wikipedia.org/wiki/Superstring_theory "Superstring theory") [Type I string](https://en.wikipedia.org/wiki/Type_I_string_theory "Type I string theory") [Type II string](https://en.wikipedia.org/wiki/Type_II_string_theory "Type II string theory") [Type IIA string](https://en.wikipedia.org/wiki/Type_II_string_theory "Type II string theory") [Type IIB string](https://en.wikipedia.org/wiki/Type_II_string_theory "Type II string theory") [Heterotic string](https://en.wikipedia.org/wiki/Heterotic_string_theory "Heterotic string theory") [N=2 superstring](https://en.wikipedia.org/wiki/N%3D2_superstring "N=2 superstring") [F-theory](https://en.wikipedia.org/wiki/F-theory "F-theory") [String field theory](https://en.wikipedia.org/wiki/String_field_theory "String field theory") [Matrix string theory](https://en.wikipedia.org/wiki/Matrix_string_theory "Matrix string theory") [Non-critical string theory](https://en.wikipedia.org/wiki/Non-critical_string_theory "Non-critical string theory") [Non-linear sigma model](https://en.wikipedia.org/wiki/Non-linear_sigma_model "Non-linear sigma model") [Tachyon condensation](https://en.wikipedia.org/wiki/Tachyon_condensation "Tachyon condensation") [RNS formalism](https://en.wikipedia.org/wiki/RNS_formalism "RNS formalism") [GS formalism](https://en.wikipedia.org/wiki/GS_formalism "GS formalism") |
| [String duality](https://en.wikipedia.org/wiki/String_duality "String duality") | [T-duality](https://en.wikipedia.org/wiki/T-duality "T-duality") [S-duality](https://en.wikipedia.org/wiki/S-duality "S-duality") [U-duality](https://en.wikipedia.org/wiki/U-duality "U-duality") [Montonen–Olive duality](https://en.wikipedia.org/wiki/Montonen%E2%80%93Olive_duality "Montonen–Olive duality") |
| Particles and fields | [Graviton](https://en.wikipedia.org/wiki/Graviton "Graviton") [Dilaton](https://en.wikipedia.org/wiki/Dilaton "Dilaton") [Tachyon](https://en.wikipedia.org/wiki/Tachyon "Tachyon") [Ramond–Ramond field](https://en.wikipedia.org/wiki/Ramond%E2%80%93Ramond_field "Ramond–Ramond field") [Kalb–Ramond field](https://en.wikipedia.org/wiki/Kalb%E2%80%93Ramond_field "Kalb–Ramond field") [Magnetic monopole](https://en.wikipedia.org/wiki/Magnetic_monopole "Magnetic monopole") [Dual graviton](https://en.wikipedia.org/wiki/Dual_graviton "Dual graviton") [Dual photon](https://en.wikipedia.org/wiki/Dual_photon "Dual photon") |
| [Branes](https://en.wikipedia.org/wiki/Brane "Brane") | [D-brane](https://en.wikipedia.org/wiki/D-brane "D-brane") [NS5-brane](https://en.wikipedia.org/wiki/NS5-brane "NS5-brane") [M2-brane](https://en.wikipedia.org/wiki/M2-brane "M2-brane") [M5-brane](https://en.wikipedia.org/wiki/M5-brane "M5-brane") [S-brane](https://en.wikipedia.org/wiki/S-brane "S-brane") [Black brane](https://en.wikipedia.org/wiki/Black_brane "Black brane") [Black holes](https://en.wikipedia.org/wiki/Black_hole "Black hole") [Black string](https://en.wikipedia.org/wiki/Black_string "Black string") [Brane cosmology](https://en.wikipedia.org/wiki/Brane_cosmology "Brane cosmology") [Quiver diagram](https://en.wikipedia.org/wiki/Quiver_diagram "Quiver diagram") [Hanany–Witten transition](https://en.wikipedia.org/wiki/Hanany%E2%80%93Witten_transition "Hanany–Witten transition") |
| [Conformal field theory](https://en.wikipedia.org/wiki/Conformal_field_theory "Conformal field theory") | [Virasoro algebra](https://en.wikipedia.org/wiki/Virasoro_algebra "Virasoro algebra") [Mirror symmetry](https://en.wikipedia.org/wiki/Mirror_symmetry_\(string_theory\) "Mirror symmetry (string theory)") [Conformal anomaly](https://en.wikipedia.org/wiki/Conformal_anomaly "Conformal anomaly") [Conformal algebra](https://en.wikipedia.org/wiki/Conformal_symmetry "Conformal symmetry") [Superconformal algebra](https://en.wikipedia.org/wiki/Superconformal_algebra "Superconformal algebra") [Vertex operator algebra](https://en.wikipedia.org/wiki/Vertex_operator_algebra "Vertex operator algebra") [Loop algebra](https://en.wikipedia.org/wiki/Loop_algebra "Loop algebra") [Kac–Moody algebra](https://en.wikipedia.org/wiki/Kac%E2%80%93Moody_algebra "Kac–Moody algebra") [Wess–Zumino–Witten model](https://en.wikipedia.org/wiki/Wess%E2%80%93Zumino%E2%80%93Witten_model "Wess–Zumino–Witten model") |
| [Gauge theory](https://en.wikipedia.org/wiki/Gauge_theory "Gauge theory") | [Anomalies](https://en.wikipedia.org/wiki/Anomaly_\(physics\) "Anomaly (physics)") [Instantons](https://en.wikipedia.org/wiki/Instanton "Instanton") [Chern–Simons form](https://en.wikipedia.org/wiki/Chern%E2%80%93Simons_form "Chern–Simons form") [Bogomol'nyi–Prasad–Sommerfield bound](https://en.wikipedia.org/wiki/Bogomol%27nyi%E2%80%93Prasad%E2%80%93Sommerfield_bound "Bogomol'nyi–Prasad–Sommerfield bound") [Exceptional Lie groups](https://en.wikipedia.org/wiki/Exceptional_Lie_group "Exceptional Lie group") ([G2](https://en.wikipedia.org/wiki/G2_\(mathematics\) "G2 (mathematics)"), [F4](https://en.wikipedia.org/wiki/F4_\(mathematics\) "F4 (mathematics)"), [E6](https://en.wikipedia.org/wiki/E6_\(mathematics\) "E6 (mathematics)"), [E7](https://en.wikipedia.org/wiki/E7_\(mathematics\) "E7 (mathematics)"), [E8](https://en.wikipedia.org/wiki/E8_\(mathematics\) "E8 (mathematics)")) [ADE classification](https://en.wikipedia.org/wiki/ADE_classification "ADE classification") [Dirac string](https://en.wikipedia.org/wiki/Dirac_string "Dirac string") [*p*\-form electrodynamics](https://en.wikipedia.org/wiki/P-form_electrodynamics "P-form electrodynamics") |
| Geometry | [Worldsheet](https://en.wikipedia.org/wiki/Worldsheet "Worldsheet") [Kaluza–Klein theory](https://en.wikipedia.org/wiki/Kaluza%E2%80%93Klein_theory "Kaluza–Klein theory") [Compactification](https://en.wikipedia.org/wiki/Compactification_\(physics\) "Compactification (physics)") [Why 10 dimensions](https://en.wikipedia.org/wiki/Why_10_dimensions "Why 10 dimensions")? [Kähler manifold](https://en.wikipedia.org/wiki/K%C3%A4hler_manifold "Kähler manifold") [Ricci-flat manifold](https://en.wikipedia.org/wiki/Ricci-flat_manifold "Ricci-flat manifold") [Calabi–Yau manifold](https://en.wikipedia.org/wiki/Calabi%E2%80%93Yau_manifold "Calabi–Yau manifold") [Hyperkähler manifold](https://en.wikipedia.org/wiki/Hyperk%C3%A4hler_manifold "Hyperkähler manifold") [K3 surface](https://en.wikipedia.org/wiki/K3_surface "K3 surface") [G2 manifold](https://en.wikipedia.org/wiki/G2_manifold "G2 manifold") [Spin(7)-manifold](https://en.wikipedia.org/wiki/Spin\(7\)-manifold "Spin(7)-manifold") [Generalized complex manifold](https://en.wikipedia.org/wiki/Generalized_complex_structure "Generalized complex structure") [Orbifold](https://en.wikipedia.org/wiki/Orbifold "Orbifold") [Conifold](https://en.wikipedia.org/wiki/Conifold "Conifold") [Orientifold](https://en.wikipedia.org/wiki/Orientifold "Orientifold") [Moduli space](https://en.wikipedia.org/wiki/Moduli_space "Moduli space") [Hořava–Witten theory](https://en.wikipedia.org/wiki/Ho%C5%99ava%E2%80%93Witten_theory "Hořava–Witten theory") [K-theory (physics)](https://en.wikipedia.org/wiki/K-theory_\(physics\) "K-theory (physics)") [Twisted K-theory](https://en.wikipedia.org/wiki/Twisted_K-theory "Twisted K-theory") |
| [Supersymmetry](https://en.wikipedia.org/wiki/Supersymmetry "Supersymmetry") | [Supergravity](https://en.wikipedia.org/wiki/Supergravity "Supergravity") [Eleven-dimensional supergravity](https://en.wikipedia.org/wiki/Eleven-dimensional_supergravity "Eleven-dimensional supergravity") [Type I supergravity](https://en.wikipedia.org/wiki/Type_I_supergravity "Type I supergravity") [Type IIA supergravity](https://en.wikipedia.org/wiki/Type_IIA_supergravity "Type IIA supergravity") [Type IIB supergravity](https://en.wikipedia.org/wiki/Type_IIB_supergravity "Type IIB supergravity") [Superspace](https://en.wikipedia.org/wiki/Superspace "Superspace") [Lie superalgebra](https://en.wikipedia.org/wiki/Lie_superalgebra "Lie superalgebra") [Lie supergroup](https://en.wikipedia.org/wiki/Lie_supergroup "Lie supergroup") |
| [Holography](https://en.wikipedia.org/wiki/Holography "Holography") | [Holographic principle](https://en.wikipedia.org/wiki/Holographic_principle "Holographic principle") [AdS/CFT correspondence](https://en.wikipedia.org/wiki/AdS/CFT_correspondence "AdS/CFT correspondence") |
| [M-theory](https://en.wikipedia.org/wiki/M-theory "M-theory") | [Matrix theory](https://en.wikipedia.org/wiki/Matrix_theory_\(physics\) "Matrix theory (physics)") [Introduction to M-theory](https://en.wikipedia.org/wiki/Introduction_to_M-theory "Introduction to M-theory") |
| String theorists | [Aganagić](https://en.wikipedia.org/wiki/Mina_Aganagi%C4%87 "Mina Aganagić") [Arkani-Hamed](https://en.wikipedia.org/wiki/Nima_Arkani-Hamed "Nima Arkani-Hamed") [Atiyah](https://en.wikipedia.org/wiki/Michael_Atiyah "Michael Atiyah") [Banks](https://en.wikipedia.org/wiki/Tom_Banks_\(physicist\) "Tom Banks (physicist)") [Berenstein](https://en.wikipedia.org/wiki/David_Berenstein "David Berenstein") [Bousso](https://en.wikipedia.org/wiki/Raphael_Bousso "Raphael Bousso") [Curtright](https://en.wikipedia.org/wiki/Thomas_Curtright "Thomas Curtright") [Dijkgraaf](https://en.wikipedia.org/wiki/Robbert_Dijkgraaf "Robbert Dijkgraaf") [Distler](https://en.wikipedia.org/wiki/Jacques_Distler "Jacques Distler") [Douglas](https://en.wikipedia.org/wiki/Michael_R._Douglas "Michael R. Douglas") [Duff](https://en.wikipedia.org/wiki/Michael_Duff_\(physicist\) "Michael Duff (physicist)") [Dvali](https://en.wikipedia.org/wiki/Gia_Dvali "Gia Dvali") [Ferrara](https://en.wikipedia.org/wiki/Sergio_Ferrara "Sergio Ferrara") [Fischler](https://en.wikipedia.org/wiki/Willy_Fischler "Willy Fischler") [Friedan](https://en.wikipedia.org/wiki/Daniel_Friedan "Daniel Friedan") [Gates](https://en.wikipedia.org/wiki/Sylvester_James_Gates "Sylvester James Gates") [Gliozzi](https://en.wikipedia.org/wiki/Ferdinando_Gliozzi "Ferdinando Gliozzi") [Gopakumar](https://en.wikipedia.org/wiki/Rajesh_Gopakumar "Rajesh Gopakumar") [Green](https://en.wikipedia.org/wiki/Michael_Green_\(physicist\) "Michael Green (physicist)") [Greene](https://en.wikipedia.org/wiki/Brian_Greene "Brian Greene") [Gross](https://en.wikipedia.org/wiki/David_Gross "David Gross") [Gubser](https://en.wikipedia.org/wiki/Steven_Gubser "Steven Gubser") [Gukov](https://en.wikipedia.org/wiki/Sergei_Gukov "Sergei Gukov") [Guth](https://en.wikipedia.org/wiki/Alan_Guth "Alan Guth") [Hanson](https://en.wikipedia.org/wiki/Andrew_J._Hanson "Andrew J. Hanson") [Harvey](https://en.wikipedia.org/wiki/Jeffrey_A._Harvey "Jeffrey A. Harvey") ['t Hooft](https://en.wikipedia.org/wiki/Gerard_%27t_Hooft "Gerard 't Hooft") [Hořava](https://en.wikipedia.org/wiki/Petr_Ho%C5%99ava_\(theorist\) "Petr Hořava (theorist)") [Gibbons](https://en.wikipedia.org/wiki/Gary_Gibbons "Gary Gibbons") [Kachru](https://en.wikipedia.org/wiki/Shamit_Kachru "Shamit Kachru") [Kaku](https://en.wikipedia.org/wiki/Michio_Kaku "Michio Kaku") [Kallosh](https://en.wikipedia.org/wiki/Renata_Kallosh "Renata Kallosh") [Kaluza](https://en.wikipedia.org/wiki/Theodor_Kaluza "Theodor Kaluza") [Kapustin](https://en.wikipedia.org/wiki/Anton_Kapustin "Anton Kapustin") [Klebanov](https://en.wikipedia.org/wiki/Igor_Klebanov "Igor Klebanov") [Knizhnik](https://en.wikipedia.org/wiki/Vadim_Knizhnik "Vadim Knizhnik") [Kontsevich](https://en.wikipedia.org/wiki/Maxim_Kontsevich "Maxim Kontsevich") [Klein](https://en.wikipedia.org/wiki/Oskar_Klein "Oskar Klein") [Linde](https://en.wikipedia.org/wiki/Andrei_Linde "Andrei Linde") 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String theory landscape
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| Readable Markdown | From Wikipedia, the free encyclopedia
In [string theory](https://en.wikipedia.org/wiki/String_theory "String theory"), the **string theory landscape** (or **landscape of vacua**) is the collection of possible [false vacua](https://en.wikipedia.org/wiki/False_vacuum "False vacuum"),[\[1\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-Ashok-1) together comprising a collective "landscape" of choices of parameters governing [compactifications](https://en.wikipedia.org/wiki/Compactification_\(physics\) "Compactification (physics)").
The term "landscape" comes from the notion of a [fitness landscape](https://en.wikipedia.org/wiki/Fitness_landscape "Fitness landscape") in [evolutionary biology](https://en.wikipedia.org/wiki/Evolutionary_biology "Evolutionary biology").[\[2\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-2) It was first applied to cosmology by [Lee Smolin](https://en.wikipedia.org/wiki/Lee_Smolin "Lee Smolin") in his book *[The Life of the Cosmos](https://en.wikipedia.org/wiki/The_Life_of_the_Cosmos "The Life of the Cosmos")* (1997), and was first used in the context of string theory by [Leonard Susskind](https://en.wikipedia.org/wiki/Leonard_Susskind "Leonard Susskind").[\[3\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-3)
## Compactified Calabi–Yau manifolds
\[[edit](https://en.wikipedia.org/w/index.php?title=String_theory_landscape&action=edit§ion=1 "Edit section: Compactified Calabi–Yau manifolds")\]
In string theory, the estimated count of distinct flux vacua is commonly stated as having a lower bound of ,[\[4\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-4) but more recently this has been revised to ,[\[5\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-5) and the true number may still be far higher. The large number of possibilities arises from choices of [Calabi–Yau manifolds](https://en.wikipedia.org/wiki/Calabi%E2%80%93Yau_manifold "Calabi–Yau manifold") and choices of generalized [magnetic fluxes](https://en.wikipedia.org/wiki/Magnetic_flux "Magnetic flux") over various [homology](https://en.wikipedia.org/wiki/Homology_\(mathematics\) "Homology (mathematics)") cycles, found in [F-theory](https://en.wikipedia.org/wiki/F-theory "F-theory").
If there is no structure in the space of vacua, the problem of finding one with a sufficiently small cosmological constant is [NP complete](https://en.wikipedia.org/wiki/NP_complete "NP complete").[\[6\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-6) This is a version of the [subset sum problem](https://en.wikipedia.org/wiki/Subset_sum_problem "Subset sum problem").
A possible mechanism of string theory vacuum stabilization, now known as the **KKLT mechanism**, was proposed in 2003 by [Shamit Kachru](https://en.wikipedia.org/wiki/Shamit_Kachru "Shamit Kachru"), [Renata Kallosh](https://en.wikipedia.org/wiki/Renata_Kallosh "Renata Kallosh"), [Andrei Linde](https://en.wikipedia.org/wiki/Andrei_Linde "Andrei Linde"), and [Sandip Trivedi](https://en.wikipedia.org/wiki/Sandip_Trivedi "Sandip Trivedi").[\[7\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-7)
## Fine-tuning by the anthropic principle
\[[edit](https://en.wikipedia.org/w/index.php?title=String_theory_landscape&action=edit§ion=2 "Edit section: Fine-tuning by the anthropic principle")\]
[Fine-tuning](https://en.wikipedia.org/wiki/Fine-tuning_\(physics\) "Fine-tuning (physics)") of constants like the [cosmological constant](https://en.wikipedia.org/wiki/Cosmological_constant "Cosmological constant") or the [Higgs boson](https://en.wikipedia.org/wiki/Higgs_boson "Higgs boson") mass is usually assumed to occur for precise physical reasons as opposed to taking their particular values at random. That is, these values should be uniquely consistent with underlying physical laws.
The number of theoretically allowed configurations has prompted suggestions\[*[according to whom?](https://en.wikipedia.org/wiki/Wikipedia:Manual_of_Style/Words_to_watch#Unsupported_attributions "Wikipedia:Manual of Style/Words to watch")*\] that this is not the case, and that many different vacua are physically realized.[\[8\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-8) The [anthropic principle](https://en.wikipedia.org/wiki/Anthropic_principle "Anthropic principle") proposes that fundamental constants may have the values they have because such values are necessary for life (and therefore intelligent observers to measure the constants). The *anthropic landscape* thus refers to the collection of those portions of the landscape that are suitable for supporting intelligent life.
In 1987, [Steven Weinberg](https://en.wikipedia.org/wiki/Steven_Weinberg "Steven Weinberg") proposed that the observed value of the [cosmological constant](https://en.wikipedia.org/wiki/Cosmological_constant "Cosmological constant") was so small because it is impossible for life to occur in a universe with a much larger cosmological constant.[\[9\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-9)
Weinberg attempted to predict the magnitude of the cosmological constant based on probabilistic arguments. Other attempts\[*[which?](https://en.wikipedia.org/wiki/Wikipedia:Avoid_weasel_words "Wikipedia:Avoid weasel words")*\] have been made to apply similar reasoning to models of particle physics.[\[10\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-10)
Such attempts are based in the general ideas of [Bayesian probability](https://en.wikipedia.org/wiki/Bayesian_probability "Bayesian probability"); interpreting probability in a context where it is only possible to draw one [sample](https://en.wikipedia.org/wiki/Sample_size "Sample size") from a [distribution](https://en.wikipedia.org/wiki/Probability_distribution "Probability distribution") is problematic in [frequentist probability](https://en.wikipedia.org/wiki/Frequentist_probability "Frequentist probability") but not in Bayesian probability, which is not defined in terms of the frequency of repeated events.
In such a framework, the probability  of observing some fundamental parameters  is given by,

where  is the prior probability, from fundamental theory, of the parameters  and  is the "anthropic selection function", determined by the number of "observers" that would occur in the universe with parameters .\[*[citation needed](https://en.wikipedia.org/wiki/Wikipedia:Citation_needed "Wikipedia:Citation needed")*\]
These probabilistic arguments are the most controversial aspect of the landscape. Technical criticisms of these proposals have pointed out that:\[*[citation needed](https://en.wikipedia.org/wiki/Wikipedia:Citation_needed "Wikipedia:Citation needed")*\]\[*[year needed](https://en.wikipedia.org/wiki/Wikipedia:Manual_of_Style/Dates_and_numbers "Wikipedia:Manual of Style/Dates and numbers")*\]
- The function  is completely unknown in string theory and may be impossible to define or interpret in any sensible probabilistic way.
- The function  is completely unknown, since so little is known about the origin of life. Simplified criteria (such as the number of galaxies) must be used as a proxy for the number of observers. Moreover, it may never be possible to compute it for parameters radically different from those of the observable universe.
### Simplified approaches
\[[edit](https://en.wikipedia.org/w/index.php?title=String_theory_landscape&action=edit§ion=4 "Edit section: Simplified approaches")\]
[Tegmark](https://en.wikipedia.org/wiki/Max_Tegmark "Max Tegmark") *et al.* have recently considered these objections and proposed a simplified anthropic scenario for [axion](https://en.wikipedia.org/wiki/Axion "Axion") [dark matter](https://en.wikipedia.org/wiki/Dark_matter "Dark matter") in which they argue that the first two of these problems do not apply.[\[11\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-11)
Vilenkin and collaborators have proposed a consistent way to define the probabilities for a given vacuum.[\[12\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-12)
A problem with many of the simplified approaches people\[*[who?](https://en.wikipedia.org/wiki/Wikipedia:Manual_of_Style/Words_to_watch#Unsupported_attributions "Wikipedia:Manual of Style/Words to watch")*\] have tried is that they "predict" a cosmological constant that is too large by a factor of 10–1000 orders of magnitude (depending on one's assumptions) and hence suggest that the cosmic acceleration should be much more rapid than is observed.[\[13\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-13)[\[14\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-14)[\[15\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-15)
Few dispute the large number of metastable vacua.\[*[citation needed](https://en.wikipedia.org/wiki/Wikipedia:Citation_needed "Wikipedia:Citation needed")*\] The existence, meaning, and scientific relevance of the anthropic landscape, however, remain controversial.\[*[further explanation needed](https://en.wikipedia.org/wiki/Wikipedia:Please_clarify "Wikipedia:Please clarify")*\]
#### Cosmological constant problem
\[[edit](https://en.wikipedia.org/w/index.php?title=String_theory_landscape&action=edit§ion=6 "Edit section: Cosmological constant problem")\]
[Andrei Linde](https://en.wikipedia.org/wiki/Andrei_Linde "Andrei Linde"), [Sir Martin Rees](https://en.wikipedia.org/wiki/Sir_Martin_Rees "Sir Martin Rees") and [Leonard Susskind](https://en.wikipedia.org/wiki/Leonard_Susskind "Leonard Susskind") advocate it as a solution to the [cosmological constant problem](https://en.wikipedia.org/wiki/Cosmological_constant_problem "Cosmological constant problem").\[*[citation needed](https://en.wikipedia.org/wiki/Wikipedia:Citation_needed "Wikipedia:Citation needed")*\]
### Weak scale supersymmetry from the landscape
\[[edit](https://en.wikipedia.org/w/index.php?title=String_theory_landscape&action=edit§ion=7 "Edit section: Weak scale supersymmetry from the landscape")\]
The string landscape ideas can be applied to the notion of weak scale supersymmetry and the Little Hierarchy problem. For string vacua which include the MSSM (Minimal Supersymmetric Standard Model) as the low energy effective field theory, all values of SUSY breaking fields are expected to be equally likely on the landscape. This led Douglas[\[16\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-16) and others to propose that the SUSY breaking scale is distributed as a power law in the landscape  where  is the number of F-breaking fields (distributed as complex numbers) and  is the number of D-breaking fields (distributed as real numbers). Next, one may impose the Agrawal, Barr, Donoghue, Seckel (ABDS) anthropic requirement[\[17\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-17) that the derived weak scale lie within a factor of a few of our measured value (lest nuclei as needed for life as we know it become unstable (the atomic principle)). Combining these effects with a mild power-law draw to large soft SUSY breaking terms, one may calculate the Higgs boson and superparticle masses expected from the landscape.[\[18\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-18) The Higgs mass probability distribution peaks around 125 GeV while sparticles (with the exception of light higgsinos) tend to lie well beyond current LHC search limits. This approach is an example of the application of stringy naturalness.
#### Scientific relevance
\[[edit](https://en.wikipedia.org/w/index.php?title=String_theory_landscape&action=edit§ion=8 "Edit section: Scientific relevance")\]
[David Gross](https://en.wikipedia.org/wiki/David_Gross "David Gross") suggests\[*[citation needed](https://en.wikipedia.org/wiki/Wikipedia:Citation_needed "Wikipedia:Citation needed")*\] that the idea is inherently unscientific, unfalsifiable or premature. A famous debate on the anthropic landscape of string theory is the [Smolin–Susskind debate](https://en.wikipedia.org/wiki/Smolin%E2%80%93Susskind_debate "Smolin–Susskind debate") on the merits of the landscape.
There are several popular books about the anthropic principle in cosmology.[\[19\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-19) The authors of two physics blogs, [Lubos Motl](https://en.wikipedia.org/wiki/Lubos_Motl "Lubos Motl") and [Peter Woit](https://en.wikipedia.org/wiki/Peter_Woit "Peter Woit"), are opposed to this use of the anthropic principle.\[*[why?](https://en.wikipedia.org/wiki/Wikipedia:Please_clarify "Wikipedia:Please clarify")*\][\[20\]](https://en.wikipedia.org/wiki/String_theory_landscape#cite_note-20)
- [Swampland](https://en.wikipedia.org/wiki/Swampland_\(physics\) "Swampland (physics)")
- [Extra dimensions](https://en.wikipedia.org/wiki/String_theory#Extra_dimensions "String theory")
- [M-theory](https://en.wikipedia.org/wiki/M-theory "M-theory")
1. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-Ashok_1-0)** The number of metastable vacua is not known exactly, but commonly quoted estimates are of the order 10500. See [M. Douglas](https://en.wikipedia.org/wiki/Michael_R._Douglas "Michael R. Douglas"), "The statistics of string / M theory vacua", *JHEP* **0305**, 46 (2003). [arXiv](https://en.wikipedia.org/wiki/ArXiv_\(identifier\) "ArXiv (identifier)"):[hep-th/0303194](https://arxiv.org/abs/hep-th/0303194); S. Ashok and M. Douglas, "Counting flux vacua", *JHEP* **0401**, 060 (2004).
2. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-2)**
Baggott, Jim (2018). [*Quantum Space Loop Quantum Gravity and the Search for the Structure of Space, Time, and the Universe*](https://books.google.com/books?id=HwN6DwAAQBAJ&pg=PA288). Oxford University Press. p. 288. [ISBN](https://en.wikipedia.org/wiki/ISBN_\(identifier\) "ISBN (identifier)")
[978-0-19-253681-5](https://en.wikipedia.org/wiki/Special:BookSources/978-0-19-253681-5 "Special:BookSources/978-0-19-253681-5")
.
3. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-3)** L. Smolin, "Did the universe evolve?", *Classical and Quantum Gravity* **9**, 173–191 (1992). L. Smolin, *[The Life of the Cosmos](https://en.wikipedia.org/wiki/The_Life_of_the_Cosmos "The Life of the Cosmos")* (Oxford, 1997)
4. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-4)**
Read, James; Le Bihan, Baptiste (2021). ["The landscape and the multiverse: What's the problem?"](https://doi.org/10.1007%2Fs11229-021-03137-0). *Synthese*. **199** (3–4\): 7749–7771\. [doi](https://en.wikipedia.org/wiki/Doi_\(identifier\) "Doi (identifier)"):[10\.1007/s11229-021-03137-0](https://doi.org/10.1007%2Fs11229-021-03137-0). [S2CID](https://en.wikipedia.org/wiki/S2CID_\(identifier\) "S2CID (identifier)") [234815857](https://api.semanticscholar.org/CorpusID:234815857).
5. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-5)**
Taylor, Washington; Wang, Yi-Nan (2015). "The F-theory geometry with most flux vacua". *Journal of High Energy Physics*. **2015** (12): 164. [arXiv](https://en.wikipedia.org/wiki/ArXiv_\(identifier\) "ArXiv (identifier)"):[1511\.03209](https://arxiv.org/abs/1511.03209). [Bibcode](https://en.wikipedia.org/wiki/Bibcode_\(identifier\) "Bibcode (identifier)"):[2015JHEP...12..164T](https://ui.adsabs.harvard.edu/abs/2015JHEP...12..164T). [doi](https://en.wikipedia.org/wiki/Doi_\(identifier\) "Doi (identifier)"):[10\.1007/JHEP12(2015)164](https://doi.org/10.1007%2FJHEP12%282015%29164). [S2CID](https://en.wikipedia.org/wiki/S2CID_\(identifier\) "S2CID (identifier)") [41149049](https://api.semanticscholar.org/CorpusID:41149049).
6. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-6)**
Frederik Denef; Douglas, Michael R. (2007). "Computational complexity of the landscape". *Annals of Physics*. **322** (5): 1096–1142\. [arXiv](https://en.wikipedia.org/wiki/ArXiv_\(identifier\) "ArXiv (identifier)"):[hep-th/0602072](https://arxiv.org/abs/hep-th/0602072). [Bibcode](https://en.wikipedia.org/wiki/Bibcode_\(identifier\) "Bibcode (identifier)"):[2007AnPhy.322.1096D](https://ui.adsabs.harvard.edu/abs/2007AnPhy.322.1096D). [doi](https://en.wikipedia.org/wiki/Doi_\(identifier\) "Doi (identifier)"):[10\.1016/j.aop.2006.07.013](https://doi.org/10.1016%2Fj.aop.2006.07.013). [S2CID](https://en.wikipedia.org/wiki/S2CID_\(identifier\) "S2CID (identifier)") [281586](https://api.semanticscholar.org/CorpusID:281586).
7. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-7)**
Kachru, Shamit; Kallosh, Renata; Linde, Andrei; Trivedi, Sandip P. (2003). "de Sitter Vacua in String Theory". *Physical Review D*. **68** (4) 046005. [arXiv](https://en.wikipedia.org/wiki/ArXiv_\(identifier\) "ArXiv (identifier)"):[hep-th/0301240](https://arxiv.org/abs/hep-th/0301240). [Bibcode](https://en.wikipedia.org/wiki/Bibcode_\(identifier\) "Bibcode (identifier)"):[2003PhRvD..68d6005K](https://ui.adsabs.harvard.edu/abs/2003PhRvD..68d6005K). [doi](https://en.wikipedia.org/wiki/Doi_\(identifier\) "Doi (identifier)"):[10\.1103/PhysRevD.68.046005](https://doi.org/10.1103%2FPhysRevD.68.046005). [S2CID](https://en.wikipedia.org/wiki/S2CID_\(identifier\) "S2CID (identifier)") [119482182](https://api.semanticscholar.org/CorpusID:119482182).
8. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-8)** L. Susskind, "The anthropic landscape of string theory", [arXiv](https://en.wikipedia.org/wiki/ArXiv_\(identifier\) "ArXiv (identifier)"):[hep-th/0302219](https://arxiv.org/abs/hep-th/0302219).
9. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-9)** S. Weinberg, "Anthropic bound on the cosmological constant", *Phys. Rev. Lett.* **59**, 2607 (1987).
10. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-10)** S. M. Carroll, "Is our universe natural?" (2005) [arXiv](https://en.wikipedia.org/wiki/ArXiv_\(identifier\) "ArXiv (identifier)"):[hep-th/0512148](https://arxiv.org/abs/hep-th/0512148) reviews a number of proposals in preprints dated 2004/5.
11. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-11)** M. Tegmark, A. Aguirre, M. Rees and F. Wilczek, "Dimensionless constants, cosmology and other dark matters", [arXiv](https://en.wikipedia.org/wiki/ArXiv_\(identifier\) "ArXiv (identifier)"):[astro-ph/0511774](https://arxiv.org/abs/astro-ph/0511774). F. Wilczek, "Enlightenment, knowledge, ignorance, temptation", [arXiv](https://en.wikipedia.org/wiki/ArXiv_\(identifier\) "ArXiv (identifier)"):[hep-ph/0512187](https://arxiv.org/abs/hep-ph/0512187). See also the discussion at [\[1\]](http://www.math.columbia.edu/~woit/wordpress/?p=310).
12. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-12)**
See, *e.g.*
Alexander Vilenkin (2007). "A measure of the multiverse". *Journal of Physics A: Mathematical and Theoretical*. **40** (25): 6777–6785\. [arXiv](https://en.wikipedia.org/wiki/ArXiv_\(identifier\) "ArXiv (identifier)"):[hep-th/0609193](https://arxiv.org/abs/hep-th/0609193). [Bibcode](https://en.wikipedia.org/wiki/Bibcode_\(identifier\) "Bibcode (identifier)"):[2007JPhA...40.6777V](https://ui.adsabs.harvard.edu/abs/2007JPhA...40.6777V). [doi](https://en.wikipedia.org/wiki/Doi_\(identifier\) "Doi (identifier)"):[10\.1088/1751-8113/40/25/S22](https://doi.org/10.1088%2F1751-8113%2F40%2F25%2FS22). [S2CID](https://en.wikipedia.org/wiki/S2CID_\(identifier\) "S2CID (identifier)") [119390736](https://api.semanticscholar.org/CorpusID:119390736).
13. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-13)**
Abraham Loeb (2006). "An observational test for the anthropic origin of the cosmological constant". *Journal of Cosmology and Astroparticle Physics*. **0605** (5): 009. [arXiv](https://en.wikipedia.org/wiki/ArXiv_\(identifier\) "ArXiv (identifier)"):[astro-ph/0604242](https://arxiv.org/abs/astro-ph/0604242). [Bibcode](https://en.wikipedia.org/wiki/Bibcode_\(identifier\) "Bibcode (identifier)"):[2006JCAP...05..009L](https://ui.adsabs.harvard.edu/abs/2006JCAP...05..009L). [doi](https://en.wikipedia.org/wiki/Doi_\(identifier\) "Doi (identifier)"):[10\.1088/1475-7516/2006/05/009](https://doi.org/10.1088%2F1475-7516%2F2006%2F05%2F009). [S2CID](https://en.wikipedia.org/wiki/S2CID_\(identifier\) "S2CID (identifier)") [39340203](https://api.semanticscholar.org/CorpusID:39340203).
14. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-14)**
Jaume Garriga & Alexander Vilenkin (2006). "Anthropic prediction for Lambda and the Q catastrophe". *Prog. Theor. Phys. Suppl*. **163**: 245–57\. [arXiv](https://en.wikipedia.org/wiki/ArXiv_\(identifier\) "ArXiv (identifier)"):[hep-th/0508005](https://arxiv.org/abs/hep-th/0508005). [Bibcode](https://en.wikipedia.org/wiki/Bibcode_\(identifier\) "Bibcode (identifier)"):[2006PThPS.163..245G](https://ui.adsabs.harvard.edu/abs/2006PThPS.163..245G). [doi](https://en.wikipedia.org/wiki/Doi_\(identifier\) "Doi (identifier)"):[10\.1143/PTPS.163.245](https://doi.org/10.1143%2FPTPS.163.245). [S2CID](https://en.wikipedia.org/wiki/S2CID_\(identifier\) "S2CID (identifier)") [118936307](https://api.semanticscholar.org/CorpusID:118936307).
15. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-15)**
Delia Schwartz-Perlov & Alexander Vilenkin (2006). "Probabilities in the Bousso-Polchinski multiverse". *Journal of Cosmology and Astroparticle Physics*. **0606** (6): 010. [arXiv](https://en.wikipedia.org/wiki/ArXiv_\(identifier\) "ArXiv (identifier)"):[hep-th/0601162](https://arxiv.org/abs/hep-th/0601162). [Bibcode](https://en.wikipedia.org/wiki/Bibcode_\(identifier\) "Bibcode (identifier)"):[2006JCAP...06..010S](https://ui.adsabs.harvard.edu/abs/2006JCAP...06..010S). [doi](https://en.wikipedia.org/wiki/Doi_\(identifier\) "Doi (identifier)"):[10\.1088/1475-7516/2006/06/010](https://doi.org/10.1088%2F1475-7516%2F2006%2F06%2F010). [S2CID](https://en.wikipedia.org/wiki/S2CID_\(identifier\) "S2CID (identifier)") [119337679](https://api.semanticscholar.org/CorpusID:119337679).
16. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-16)** M. R. Douglas, "Statistical analysis of the supersymmetry breaking scale", [arXiv](https://en.wikipedia.org/wiki/ArXiv_\(identifier\) "ArXiv (identifier)"):[hep-th/0405279](https://arxiv.org/abs/hep-th/0405279).
17. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-17)** V. Agrawal, S. M. Barr, J. F. Donoghue and D. Seckel, "Anthropic considerations in multiple domain theories and the scale of electroweak symmetry breaking", *Phys. Rev. Lett.* **80**, 1822 (1998).[arXiv](https://en.wikipedia.org/wiki/ArXiv_\(identifier\) "ArXiv (identifier)"):[hep-ph/9801253](https://arxiv.org/abs/hep-ph/9801253)
18. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-18)** H. Baer, V. Barger, H. Serce and K. Sinha, "Higgs and superparticle mass predictions from the landscape", *JHEP* **03**, 002 (2018), [arXiv](https://en.wikipedia.org/wiki/ArXiv_\(identifier\) "ArXiv (identifier)"):[1712\.01399](https://arxiv.org/abs/1712.01399) .
19. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-19)** L. Susskind, *The cosmic landscape: string theory and the illusion of intelligent design* (Little, Brown, 2005). M. J. Rees, *Just six numbers: the deep forces that shape the universe* (Basic Books, 2001). R. Bousso and J. Polchinski, "The string theory landscape", *Sci. Am.* **291**, 60–69 (2004).
20. **[^](https://en.wikipedia.org/wiki/String_theory_landscape#cite_ref-20)** Motl's blog criticized the anthropic principle and Woit's [blog](http://www.math.columbia.edu/~woit/blog/) frequently attacks the anthropic string landscape.
- [String landscape; moduli stabilization; flux vacua; flux compactification](http://xstructure.inr.ac.ru/x-bin/theme2.py?arxiv=hep-th&level=1&index1=5460697) on [arxiv.org](https://en.wikipedia.org/wiki/Arxiv.org "Arxiv.org").
- [Cvetič, Mirjam](https://en.wikipedia.org/wiki/Mirjam_Cveti%C4%8D "Mirjam Cvetič"); García-Etxebarria, Iñaki; Halverson, James (March 2011). "On the computation of non-perturbative effective potentials in the string theory landscape". *Fortschritte der Physik*. **59** (3–4\): 243–283\. [arXiv](https://en.wikipedia.org/wiki/ArXiv_\(identifier\) "ArXiv (identifier)"):[1009\.5386](https://arxiv.org/abs/1009.5386). [Bibcode](https://en.wikipedia.org/wiki/Bibcode_\(identifier\) "Bibcode (identifier)"):[2011ForPh..59..243C](https://ui.adsabs.harvard.edu/abs/2011ForPh..59..243C). [doi](https://en.wikipedia.org/wiki/Doi_\(identifier\) "Doi (identifier)"):[10\.1002/prop.201000093](https://doi.org/10.1002%2Fprop.201000093). [S2CID](https://en.wikipedia.org/wiki/S2CID_\(identifier\) "S2CID (identifier)") [46634583](https://api.semanticscholar.org/CorpusID:46634583). |
| Shard | 152 (laksa) |
| Root Hash | 17790707453426894952 |
| Unparsed URL | org,wikipedia!en,/wiki/String_theory_landscape s443 |