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M-theory and quantum fields
Seok Kim
(Seoul National University)
Colloquium, USTC, Hefei
June 1, 2018
Quantum field theory (QFT)
• Field: physical quantities spread over space ~ wave
• Quantum fields:
- Quantum physics governs microscopic world.
- So one often needs to quantize fields.
- For instance, quantized electromagnetic fields
- Or, quantized phonons (waves of lattice vibrations)
- And so on…
• QFT is a culmination of modern physics
- “Quantum field” is a very universal notion
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QFT & string theory: 20th century
• QFT: Developed for particle physics. Almost all matters & interactions.
• String theory: includes quantum gravity
• QFT construction is flexible ↔ String theory is hard to construct.
(Lagrangian field theory)
• QFT “well understood” ↔ String theory not even well formulated.
- Can’t “solve” difficult QFTs, but it always happens in physics. (e.g. 3-body problem)
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QFT & string theory: 21st century
• Deeper studies of string theory reveal different stories.
- Novel QFTs found from string & M-theory:
novel Lagrangians, or no known Lagrangians
- duality between string theory & QFT
AdS/CFT [Maldacena]
• Needs re-interpretation of quantum fields.
- Notion of particle is emergent in QFT: in principle may not exist
- QFT often hosts emergent physics, esp. at strong coupling
• Often, ignorance on string theory ~ ignorance on QFT.
- Where we thought we understood physics but just couldn’t compute
- This feature will be more extreme in M-theory (~ strong coupling limit of strings)
4
Plan of this talk
5
String/M-theory Quantum field theory
New insights, often beyond current (Lagrangian) techniques
Triggers QFT developments
New advances in QFT enable concrete studies of string/M-theory & quantum gravity
E.g. physics of black holes
Naïve way to QFT from strings
• So how can string theory provide ground-breaking insights to QFT?
• Often obtains quantum fields at low E.
- Closed strings: contains gravity, Einstein’s general relativity
- Open strings: contains quarks & gluons
gauge theory ~ Yang-Mills theory (e.g. SU(N)),
All d.o.f. are 𝑁 ×𝑁 matrices
𝑁 D-brane boundaries
• Gauge theory is the natural QFT for string theory, as is general relativity.
• Quantum fields engineered this way: “part” of string theory, in general.
- Reflects the physics of string theory, so provides useful but limited tools.
- But in a delicate set-up, QFT is identical to strings. Provides a systematic way to study it.
6
Strings from quantum fields
• A main example: “AdS/CFT duality” or “gauge/gravity duality”
Some QFT in d dimension = Strings in a curved spacetime in d+1 dimension
(Anti – de Sitter (AdS) spacetime)
[Maldacena] 1997
• Strong coupling QFTs can be for strings (not particles)
• A realization of “holographic” gravity [‘t Hooft] [Susskind]
• Strong coupling QFT questions studied via strings & gravity
- Holographic QCD, condensed matter systems, …
• Quantum gravity questions well posed using quantum fields.
- Emergent spacetime, microscopic thermodynamics of black holes (later), …7
M-theory
• M-theory: strong coupling limits of string theories [Hull, Townsend] [Witten ‘95]
- 10d → 11d. soliton particles (“D0-branes”) ~ momenta. Emergent space at strong coupling
- String theory: Has coupling constants. Perturbation theory.
- M-theory: no tunable coupling parameters. Strong coupling. Challenge for ~ 20 years
• Completely new way of thinking of string theory & quantum gravity.
• Also provides completely new visions on QFT (than gauge theories)
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Σ10
n D0-branes
n units of KK momenta
Quantum fields from M-theory
• M-theory has two extended objects: replace strings & other extended objects
- M2-brane ~ membrane: fundamental string (wrapped on M-theory circle)
… and so on…
- M5-brane: D4-brane (wrapped on circle), NS5-brane (unwrapped)
• Challenge to QFT:
- M-theory predicts strongly interacting d=2+1 & d=5+1 QFTs on these branes.
• The challenges are posed in two different ways.
- M2-brane: demands better understanding of QFT at strong coupling (like QCD)
- M5-brane: demands new formulations of QFT, beyond the current one
• These two examples drastically enhanced (or will enhance) our notions of strong
coupling QFT.
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M2 QFTs & challenges
• 2+1d: Yang-Mills(+matters) theories at low E ~ strong coupling (“RG flow”)
- Describes M2-brane dynamics at strong coupling.
- Classical matrix-like dynamics is wiped out at strong coupling: new emergent physics
E.g. [Bagger, Lambert], [Gustavsson] (2007); [Aharony-Bergman-Jafferis-Maldacena] (2008), ……
• E.g. large 𝑁 black membrane solution predicts shocking emergent physics
- Many physical quantities scale like ∼ 𝑁3/2, rather than ∼ 𝑁2.
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E ~ gYM2 E >> gYM
2E << gYM2
weakly interacting
IR fixed point
“M2-brane QFT”
Yang-Mills-type QFTs
• M5-brane QFTs in 5+1d is much harder.
- No microscopic formulation known.
- Profound implications to lower dimensional QFTs via compactification: “M-theory of QFTs”
- E.g. on T2 : 𝑆𝐿(2, 𝑍) and Montonen-Olive electromagnetic duality
- Other Riemann surfaces: more nontrivial 4d QFTs
[Gaiotto] et.al. (2009)
• 𝑁 black M5-branes, etc. : 𝑁3 degrees of freedom
- Much more than Yang-Mills theory
- Presumably demands new structures
M5 QFTs & challenges
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= coupling constant of Yang-Millscomplex structure 𝜏 =𝜃
2𝜋+
4𝜋𝑖
𝑔𝑌𝑀2
Real challenge: QFTs in 𝑑 > 4…?
Consistent interacting QFT in d>4 is unexpected in traditional QFT.
Classical particle: 1d path. Hard to make contact interactions in higher d.
Even after quantum fluctuations, particles rarely interact in higher dimension.
Quantum particles interact in 𝑑 ≤ 3 + 1 .
In 𝑑 > 3 + 1, interacting QFTs presumably aren’t for particles.
No known models in textbooks.
(E.g. QFTs may be for “strings” in d=6.)
These examples will completely change
the intrinsic meaning of QFT.
open membrane
5-branes
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Summary of challenges & advances
• Novel # of degrees of freedom: 𝑁3/2 or 𝑁3. Either
- suggests novel emergent phenomena of gauge theories, or
- Demands new formulations of QFT
• Some physics understood from advances in strong coupling QFT tools. E.g.
- Entanglement entropy of 3d vacuum ∝ 𝑁3/2 [Drukker, Marino, Putrov] [Klebanov et.al.] (2011)
- Vacuum energy of M5 QFT ∝ 𝑁3: [H.-C. Kim, SK] [Kallen, Minahan, Nedeline, Zabzine] (2012)
- Reconstruction of AdS4 & AdS7 graviton spectra from QFTs [SK] 2009, [H.-C.Kim, SK] 2012
- And so on …
- But in d>4, only relied on string/M-theory tools or effective field theory techniques.
- So still, one needs to find a completely new approach to such systems. (E.g. New
Lagrangians, new notion of gauge symmetry, non-Lagrangian techniques for QFT, etc.)
• Recent advances in QFT techniques managed to partly catch up with string M-
theory visions on QFT. 13
Quantum gravity from QFT?
• Now, can we now use the developed notions/techniques of QFT to provide new
& useful insights to quantum gravity & strings?
• Yes.
• I’ll focus on the use of QFT in the context of AdS/CFT duality
• So many interesting achievements on QFT → QG…
- Exact spectrum of strings using “integrability” of large N QFT
[Minahan, Zarembo, Staudacher, Beisert, ………]
- Holographic gravity using entanglement, quantum information, …
- ……
- Microscopic studies of black holes in AdS space
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Black holes & QFT
• Hawking-Page phase transition (1983)
• In QFT, confinement / deconfinement phase transition [Witten] 1998
• Qualitative aspects of this transition studied from weakly-coupled gauge theory
[Aharony, Marsano, Minwalla, Papadodimas, Raamsdonk] 2003 , … 15
thermal graviton gas in AdS: 𝑇 < 𝑇𝑐 ∼ 1/𝑅𝐴𝑑𝑆
Black hole in AdS: 𝑇 > 𝑇𝑐 ∼ 1/𝑅𝐴𝑑𝑆
transition at 𝑇 = 𝑇𝑐
confined quarks/gluons ~ gravitons plasma of quark/gluon ~ black hole
transition at 𝑇 = 𝑇𝑐
A 4d Hawking-Page transition from 3d QFT
• 2+1d M2-brane QFT: vortex solitons
- Gauge theories have such objects. [Abrikosov, Nielsen, Olesen]
- In weakly-coupled Yang-Mills: heavier than 𝑁2 elementary d.o.f.
- We study partition function of “vortex” solitons on 𝑅2+1.
• “Confining” phase: vortex mass > than other mass scales (other chemical potentials)
- Large N free energy ∼ 𝑂(𝑁0): confined phase of “gravitons”
• Novel “deconfining” phase: light vortices, emergent 𝑁3/2 d.o.f.
• Gauge theory solitons provide such a mechanism in 2+1d QFT.
[Studied from so-called “Witten index” for “BPS vortices”] [Choi, Hwang, SK] to appear.
16
𝛽, 𝑇1,2,3,4 are chemical potentials
for energy & internal symmetries
Black holes from QFT: quantitative
• QFT on (sphere) x R: study their thermal free energies
• Black holes which may be understood more easily
- “Supersymmetric” black holes:
lightest black holes w/ given electric charges & spins
- Where we first microscopically understood black holes.
[Strominger, Vafa] 1996
- E.g., in AdS5 or AdS7 (related to 4d, 6d QFTs) [Gutowski, Reall, et.al], [Cvetic, et.al.]
- Their entropies are obtained from the following free energies [Zaffaroni et.al.] 2017, 2018
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black hole
𝑀 ≥1
𝑅𝐴𝑑𝑆(# σ𝐼𝑄𝐼 + # σ𝑖 𝐽𝑖)
𝑀 ≥1
𝑅𝐴𝑑𝑆(𝑄1 + 𝑄2 + 𝑄3 + 𝐽1 + 𝐽2)
𝑀 ≥1
𝑅𝐴𝑑𝑆(2𝑄1 + 2𝑄2 + 𝐽1 + 𝐽2 + 𝐽3)
string theory on 𝐴𝑑𝑆5 × 𝑆5
M-theory on 𝐴𝑑𝑆7 × 𝑆4very complicated solutions …
𝑆𝐵𝐻 =𝑁2
2
Δ1Δ2Δ3𝜔1𝜔2
+ 𝑄𝐼Δ𝐼 +𝜔𝑖𝐽𝑖
𝑆𝐵𝐻 =𝑁3
24
Δ1Δ22
𝜔1𝜔2𝜔3+ 𝑄𝐼Δ𝐼 +𝜔𝑖𝐽𝑖
𝐴𝑑𝑆5 × 𝑆5
𝐴𝑑𝑆7 × 𝑆4
Legendre transformation w/ constraint σ𝐼 Δ𝐼 − σ𝑖𝜔𝑖 = 2𝜋𝑖
Black holes from anomalies
• For 𝐴𝑑𝑆2𝑛+1=𝑜𝑑𝑑, exact “chiral anomalies” of even dimensional QFTs can be
used to study various physics at strong coupling. [Adler, Bell, Jackiw] 1969, ……
• QFT effective action on 𝑆2𝑛−1 encoding these anomalies
[Minwalla et.al.] [Komargodski et.al.] [SK, Nahmgoong]
• This computes these entropy functions from QFT, thus counting supersymmetric
AdS5 and AdS7 black holes [J.Kim, SK, Nahmgoong] to appear, [SK, Nahmgoong] 2017
• For 4d QFT, also developing a QFT model of understanding their microstates,
called “Fermi liquid model” [Berkooz, Reichmann, Simon] 2006, [Berkooz, Reichmann]18
𝜕𝜇𝑗𝜇
𝐴𝜇
𝐴𝜇
𝜕𝜇𝑗𝜇 ∼ 𝜖𝜇𝜈𝜌𝜎𝐹𝜇𝜈𝐹𝜌𝜎
−log 𝑍 =𝑁2
2
Δ1Δ2Δ3𝜔1𝜔2
−log 𝑍 =𝑁3
24
Δ1Δ22
𝜔1𝜔2𝜔3𝐴𝑑𝑆5 × 𝑆5 𝐴𝑑𝑆7 × 𝑆4
Perspectives: string theory & QFT
• String theory reveals that QFT is going far beyond the dynamics of particles.
- Various emergent phenomena: new d.o.f., strings, gravity, …
• M-theory branes have been posing special challenges to QFT.
- M2 & M5-branes: insights beyond traditional gauge theories.
- New emergent aspects of gauge theories. Needs new QFT formulations.
• QFT techniques provide insights back to string/M-theory & quantum gravity.
- Challenging problems in quantum gravity. Microscopic studies of black holes
- Many incomplete methods so far. Wild & sometimes crude (but working) ideas
- Excellent laboratory for developing some of the most challenging problems in physics…!
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