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Journal articles on the topic 'Matrix String Theory'

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Published: 14 March 2023

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1

Dijkgraaf, Robbert, Erik Verlinde, and Herman Verlinde. "Matrix string theory." Nuclear Physics B 500, no. 1-3 (September 1997): 43–61. http://dx.doi.org/10.1016/s0550-3213(97)00326-x.

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2

Bonelli, G., L. Bonora, and F. Nesti. "String interactions from Matrix string theory." Nuclear Physics B 538, no. 1-2 (January 1999): 100–116. http://dx.doi.org/10.1016/s0550-3213(98)00729-9.

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3

Brecher, D., B. Janssen, and Y. Lozano. "Dielectric fundamental strings in matrix string theory." Nuclear Physics B 634, no. 1-2 (July 2002): 23–50. http://dx.doi.org/10.1016/s0550-3213(02)00344-9.

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4

Lowe, David A. "Heterotic matrix string theory." Physics Letters B 403, no. 3-4 (June 1997): 243–49. http://dx.doi.org/10.1016/s0370-2693(97)00521-2.

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5

Berkooz, Micha, and Moshe Rozali. "String dualities from Matrix theory." Nuclear Physics B 516, no. 1-2 (April 1998): 229–40. http://dx.doi.org/10.1016/s0550-3213(97)00814-6.

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6

TSEYTLIN, A. A. "STRING THEORY EFFECTIVE ACTION: STRING LOOP CORRECTIONS." International Journal of Modern Physics A 03, no. 02 (February 1988): 365–95. http://dx.doi.org/10.1142/s0217751x88000138.

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We discuss the general ideology of the computation of string loop corrections to the effective action for the massless modes of the string. Both the S-matrix and the sigma-model approaches are presented. It is emphasized that the effective action is a more general and better defined object than the S-matrix. In particular, it is finite in spite of modular infinities that may be present in loop amplitudes computed near a “wrong” vacuum. The case of the disc topology in the open-closed string theory is treated in some detail. Some issues concerning the soft dilaton vertex operators related to the infinities of the string amplitudes are disucssed.
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7

Hosomichi, Kazuo, and Yuji Sugawara. "Multi-strings on AdS3 × S3 from matrix string theory." Journal of High Energy Physics 1999, no. 07 (July 29, 1999): 027. http://dx.doi.org/10.1088/1126-6708/1999/07/027.

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8

Bonelli, Giulio. "Matrix string theory on pp-waves." Classical and Quantum Gravity 20, no. 12 (May 20, 2003): S433—S440. http://dx.doi.org/10.1088/0264-9381/20/12/308.

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9

Morales, Jose F., and Henning Samtleben. "Supergravity Duals of Matrix String Theory." Journal of High Energy Physics 2002, no. 08 (August 27, 2002): 042. http://dx.doi.org/10.1088/1126-6708/2002/08/042.

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10

Ito, Kei, and Nobuhito Maru. "Matrix string theory from brane configuration." Physics Letters B 426, no. 1-2 (April 1998): 43–49. http://dx.doi.org/10.1016/s0370-2693(98)00274-3.

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11

Cederwall, Martin. "Open and Winding Membranes, Affine Matrix Theory and Matrix String Theory." Journal of High Energy Physics 2002, no. 12 (December 3, 2002): 005. http://dx.doi.org/10.1088/1126-6708/2002/12/005.

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12

Lowe, David A., Horatiu Nastase, and Sanjaye Ramgoolam. "Massive IIA string theory and Matrix theory compactification." Nuclear Physics B 667, no. 1-2 (September 2003): 55–89. http://dx.doi.org/10.1016/s0550-3213(03)00547-9.

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13

Uehara, Shozo, and Satoshi Yamada. "On the strong coupling region in quantum matrix string theory." Journal of High Energy Physics 2002, no. 09 (September 6, 2002): 019. http://dx.doi.org/10.1088/1126-6708/2002/09/019.

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14

Garousi, Mohammad R., and G. R. Maktabdaran. "Closed String S-matrix Elements in Open String Field Theory." Journal of High Energy Physics 2005, no. 03 (March 19, 2005): 048. http://dx.doi.org/10.1088/1126-6708/2005/03/048.

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15

KAWAI, HIKARU, and MATSUO SATO. "PERTURBATIVE VACUA FROM IIB MATRIX MODEL." International Journal of Modern Physics A 23, no. 14n15 (June 20, 2008): 2279–80. http://dx.doi.org/10.1142/s0217751x08041086.

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It has not been clarified whether a matrix model can describe various vacua of string theory. In this talk, we show that the IIB matrix model includes type IIA string theory1. In the naive large N limit of the IIB matrix model, configurations consisting of simultaneously diagonalizable matrices form a moduli space, although the unique vacuum would be determined by complicated dynamics. This moduli space should correspond to a part of perturbatively stable vacua of string theory. Actually, one point on the moduli space represents type IIA string theory. Instead of integrating over the moduli space in the path-integral, we can consider each of the simultaneously diagonalizable configurations as a background and set the fluctuations of the diagonal elements to zero. Such procedure is known as quenching in the context of the large N reduced models. By quenching the diagonal elements of the matrices to an appropriate configuration, we show that the quenched IIB matrix model is equivalent to the two-dimensional large N [Formula: see text] super Yang-Mills theory on a cylinder. This theory is nothing but matrix string theory and is known to be equivalent to type IIA string theory. As a result, we find the manner to take the large N limit in the IIB matrix model.
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16

DAS, SUMIT R., and ANTAL JEVICKI. "STRING FIELD THEORY AND PHYSICAL INTERPRETATION OF D=1 STRINGS." Modern Physics Letters A 05, no. 21 (August 30, 1990): 1639–50. http://dx.doi.org/10.1142/s0217732390001888.

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We describe a field theoretic formulation for one-dimensional string theory. It is given by the collective field representation of the matrix model and leads to a physical interpretation of the theory as that of a massless scalar field in two dimensions. The additional dimension, coming from the large-N color of the matrix model, has an extent which goes to infinity in the continuum limit. The interactions of the field theory are non-zero only at the boundaries of this additional dimension.
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17

Brax, Philippe. "The supermoduli space of matrix string theory." Journal of High Energy Physics 2000, no. 07 (July 11, 2000): 020. http://dx.doi.org/10.1088/1126-6708/2000/07/020.

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18

Silva, Pedro J. "Matrix string theory and the Myers effect." Journal of High Energy Physics 2002, no. 02 (February 5, 2002): 004. http://dx.doi.org/10.1088/1126-6708/2002/02/004.

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19

Ashoorioon, A., H. Firouzjahi, and M. M. Sheikh-Jabbari. "Matrix Inflation and its String Theory Origins." Journal of Physics: Conference Series 259 (November 1, 2010): 012031. http://dx.doi.org/10.1088/1742-6596/259/1/012031.

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20

Carqueville, Nils. "Matrix factorisations and open topological string theory." Journal of High Energy Physics 2009, no. 07 (July 2, 2009): 005. http://dx.doi.org/10.1088/1126-6708/2009/07/005.

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21

Alexandrov, Sergei Yu, Vladimir A. Kazakov, and Ivan K. Kostov. "2D string theory as normal matrix model." Nuclear Physics B 667, no. 1-2 (September 2003): 90–110. http://dx.doi.org/10.1016/s0550-3213(03)00546-7.

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22

Bonelli, G., L. Bonora, F. Nesti, and A. Tomasiello. "Matrix string theory and its moduli space." Nuclear Physics B 554, no. 1-2 (August 1999): 103–35. http://dx.doi.org/10.1016/s0550-3213(99)00271-0.

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23

Peñialba, Jesús Puente. "Non-perturbative thermodynamics in Matrix string theory." Nuclear Physics B 556, no. 1-2 (September 1999): 152–76. http://dx.doi.org/10.1016/s0550-3213(99)00388-0.

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24

Bonelli, G., L. Bonora, F. Nesti, and A. Tomasiello. "Heterotic matrix string theory and Riemann surfaces." Nuclear Physics B 564, no. 1-2 (January 2000): 86–102. http://dx.doi.org/10.1016/s0550-3213(99)00510-6.

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25

Fukuma, Masafumi, Hikaru Kawai, Yoshihisa Kitazawa, and Asato Tsuchiya. "String field theory from IIB matrix model." Nuclear Physics B - Proceedings Supplements 68, no. 1-3 (November 1998): 153–64. http://dx.doi.org/10.1016/s0920-5632(98)00149-2.

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26

Berkooz, Micha. "String dualities from matrix theory: A summary." Nuclear Physics B - Proceedings Supplements 68, no. 1-3 (November 1998): 374–80. http://dx.doi.org/10.1016/s0920-5632(98)00172-8.

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27

MINAHAN, JOSEPH A. "MATRIX MODELS AND ONE-DIMENSIONAL OPEN STRING THEORY." International Journal of Modern Physics A 08, no. 20 (August 10, 1993): 3599–614. http://dx.doi.org/10.1142/s0217751x93001466.

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We propose a random matrix model as a representation for D = 1 open strings. We show that the model with one flavor of boundary fields is equivalent to N fermions with spin in a central potential that also includes a long-range ferromagnetic interaction between the fermions that falls off as 1/(rij)2. We also generalize this theory to contain an arbitrary number of flavors. For an appropriate choice of the matrix model potential the ground state of the system can be found. Using this potential, we calculate the free energy in the double scaling limit and show that the free energy expansion has the expected form for a theory of open and closed strings if the boundary field mass and couplings have a logarithmic divergence. We then examine the critical properties of this theory and show that the length of the boundary around a hole remains finite, even near the critical point. We also argue that unlike critical string theory or a D = 0 theory, the open string coupling constant is a free parameter.
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28

Brecher, Dominic, Bert Janssen, and Yolanda Lozano. "Chern-Simons couplings for dielectric F-strings in matrix string theory." Fortschritte der Physik 50, no. 8-9 (September 2002): 864–70. http://dx.doi.org/10.1002/1521-3978(200209)50:8/9<864::aid-prop864>3.0.co;2-j.

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29

DASS, N. D. HARI, and B. SATHIAPALAN. "INTERACTION OF F- andD-STRINGS IN THE MATRIX MODEL." Modern Physics Letters A 13, no. 12 (April 20, 1998): 921–36. http://dx.doi.org/10.1142/s0217732398001005.

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We study a configuration of a parallel F- (fundamental) and D-string in IIB string theory by considering its T-dual configuration in the matrix model description of M-theory. We show that certain nonperturbative features of string theory such as O(e-1/gs) effects due to soliton loops, the existence of bound state (1,1) strings and manifest S-duality, can be seen in matrix models. We discuss certain subtleties that arise in the large-N limit when membranes are wrapped around compact dimensions.
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30

SEN, ASHOKE. "OPEN-CLOSED DUALITY: LESSONS FROM MATRIX MODEL." Modern Physics Letters A 19, no. 11 (April 10, 2004): 841–53. http://dx.doi.org/10.1142/s0217732304013581.

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Recent investigations involving the decay of unstable D-branes in string theory suggest that the tree level open string theory which describes the dynamics of the D-brane already knows about the closed string states produced in the decay of the brane. We propose a specific conjecture involving quantum open string field theory to explain this classical result, and show that the recent results in two-dimensional string theory are in exact accordance with this conjecture.
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31

SUGINO, FUMIHIKO. "COHOMOLOGICAL FIELD THEORY APPROACH TO MATRIX STRINGS." International Journal of Modern Physics A 14, no. 25 (October 10, 1999): 3979–4002. http://dx.doi.org/10.1142/s0217751x99001871.

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In this paper we consider IIA and IIB matrix string theories which are defined by two-dimensional and three-dimensional super Yang–Mills theory with the maximal supersymmetry, respectively. We exactly compute the partition function of both of the theories by mapping to a cohomological field theory. Our result for the IIA matrix string theory coincides with the result obtained in the infrared limit by Kostov and Vanhove, and thus gives a proof of the exact quasiclassics conjectured by them. Further, our result for the IIB matrix string theory coincides with the exact result of IKKT model by Moore, Nekrasov and Shatashvili. It may be an evidence of the equivalence between the two distinct IIB matrix models arising from different roots.
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32

Takayanagi, Tadashi, and Seiji Terashima. "c= 1 matrix model from string field theory." Journal of High Energy Physics 2005, no. 06 (June 28, 2005): 074. http://dx.doi.org/10.1088/1126-6708/2005/06/074.

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33

Vázquez, Samuel E. "BPS condensates, matrix models and emergent string theory." Journal of High Energy Physics 2007, no. 01 (January 30, 2007): 101. http://dx.doi.org/10.1088/1126-6708/2007/01/101.

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34

DeWolfe, Oliver, Radu Roiban, Marcus Spradlin, Anastasia Volovich, and Johannes Walcher. "On theS-matrix of type-0 string theory." Journal of High Energy Physics 2003, no. 11 (November 7, 2003): 012. http://dx.doi.org/10.1088/1126-6708/2003/11/012.

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35

Fukuma, M. "String field theory from the IIB matrix model." Nuclear Physics B 510, no. 1-2 (January 19, 1998): 158–74. http://dx.doi.org/10.1016/s0550-3213(97)00584-1.

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36

Wynter, Thomas. "Gauge fields and interactions in matrix string theory." Physics Letters B 415, no. 4 (December 1997): 349–57. http://dx.doi.org/10.1016/s0370-2693(97)01278-1.

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37

Masafumi, Fukuma, Kawai Hikaru, Kitazawa Yoshihisa, and Tsuchiya Asato. "String field theory from the IIB matrix model." Nuclear Physics B 510, no. 1-2 (January 1998): 158–74. http://dx.doi.org/10.1016/s0550-3213(98)81008-0.

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38

Wynter, Thomas. "High energy scattering amplitudes in Matrix string theory." Nuclear Physics B 580, no. 1-2 (July 2000): 147–92. http://dx.doi.org/10.1016/s0550-3213(00)00168-1.

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39

Moore, Gregory, M. Ronen Plesser, and Sanjaye Ramgoolam. "Exact S-matrix for two-dimensional string theory." Nuclear Physics B 377, no. 1-2 (June 1992): 143–90. http://dx.doi.org/10.1016/0550-3213(92)90020-c.

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40

Cohn, J. D., and S. P. De Alwis. "String field theory for d ⩽ 1 matrix models." Nuclear Physics B 368, no. 1 (January 1992): 79–97. http://dx.doi.org/10.1016/0550-3213(92)90198-k.

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41

Brustein, Ram, Dennis Nemeschansky, and Shimon Yankielowicz. "Beta functions and S-matrix in string theory." Nuclear Physics B 301, no. 2 (May 1988): 224–46. http://dx.doi.org/10.1016/0550-3213(88)90343-4.

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42

Bonora, L., and C. S. Xiong. "Two-matrix model and c = 1 string theory." Physics Letters B 347, no. 1-2 (March 1995): 41–48. http://dx.doi.org/10.1016/0370-2693(95)00153-c.

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43

Okuyama, Kazumi, and Yuji Sugawara. "Fractional strings in (p,q) 5-brane and quiver matrix string theory." Journal of High Energy Physics 1998, no. 08 (August 16, 1998): 002. http://dx.doi.org/10.1088/1126-6708/1998/08/002.

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44

DEMETERFI, KREŠIMIR. "TWO-DIMENSIONAL QUANTUM GRAVITY, MATRIX MODELS AND STRING THEORY." International Journal of Modern Physics A 08, no. 07 (March 20, 1993): 1185–244. http://dx.doi.org/10.1142/s0217751x93000497.

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We review some results of the recent progress in understanding two-dimensional quantum gravity and low-dimensional string theories based on the lattice approach. The possibility to solve the lattice models exactly comes from their equivalence to large N matrix models. We describe various matrix models and their continuum limits, and discuss in some detail the phase structure of Hermitian one-matrix models. For the one-dimensional matrix model we discuss its field theoretic formulation through a collective field method and summarize some perturbative results. We compare the results obtained from matrix models to the results in the continuum approach to string theory.
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45

Billò, M., M. Caselle, A. D'Adda, and P. Provero. "Generalized two-dimensional Yang-Mills theory is a matrix string theory." Nuclear Physics B - Proceedings Supplements 88, no. 1-3 (June 2000): 142–51. http://dx.doi.org/10.1016/s0920-5632(00)00762-3.

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46

SENGUPTA, ANIRVAN M., and SPENTA R. WADIA. "EXCITATIONS AND INTERACTIONS IN d=1 STRING THEORY." International Journal of Modern Physics A 06, no. 11 (May 10, 1991): 1961–84. http://dx.doi.org/10.1142/s0217751x91000988.

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We discuss the singlet sector of the d=1 matrix model in terms of a Dirac fermion formalism. The leading order two- and three-point functions of the density fluctuations are obtained by this method. This allows us to construct the effective action to that order and hence provide the equation of motion. This equation is compared with the one obtained from the continuum approach. We also compare continuum results for correlation functions with the matrix model ones and discuss the nature of gravitational dressing for this regularization. Finally, we address the question of boundary conditions within the framework of the d=1 unitary matrix model, considered as a regularized version of the Hermitian model, and study the implications of a generalized action with an additional parameter (analogous to the θ parameter) which give rise to quasi-periodic wave functions.
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47

Bonora, L., and C. S. Xiong. "Matrix Models, Topological Field Theories andc≤1 String Theory." Progress of Theoretical Physics Supplement 118 (1995): 201–40. http://dx.doi.org/10.1143/ptps.118.201.

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48

Lechtenfeld, Olaf, and Christian Sämann. "Matrix models and D-branes in twistor string theory." Journal of High Energy Physics 2006, no. 03 (March 2, 2006): 002. http://dx.doi.org/10.1088/1126-6708/2006/03/002.

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49

Ling, Henry, Ali Reza Mohazab, Hsien-Hang Shieh, Greg van Anders, and Mark Van Raamsdonk. "Little string theory from a double-scaled matrix model." Journal of High Energy Physics 2006, no. 10 (October 6, 2006): 018. http://dx.doi.org/10.1088/1126-6708/2006/10/018.

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50

Wynter, Thomas. "Anomalies and large N limits in matrix string theory." Physics Letters B 439, no. 1-2 (October 1998): 37–45. http://dx.doi.org/10.1016/s0370-2693(98)01028-4.

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