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UvA-DARE is a service provided by the library of the University of Amsterdam (http://dare.uva.nl) UvA-DARE (Digital Academic Repository) Supersymmetric lattice models: Field theory correspondence, integrability, defects and degeneracies Fokkema, T.B. Link to publication Citation for published version (APA): Fokkema, T. B. (2016). Supersymmetric lattice models: Field theory correspondence, integrability, defects and degeneracies. General rights It is not permitted to download or to forward/distribute the text or part of it without the consent of the author(s) and/or copyright holder(s), other than for strictly personal, individual use, unless the work is under an open content license (like Creative Commons). Disclaimer/Complaints regulations If you believe that digital publication of certain material infringes any of your rights or (privacy) interests, please let the Library know, stating your reasons. In case of a legitimate complaint, the Library will make the material inaccessible and/or remove it from the website. Please Ask the Library: https://uba.uva.nl/en/contact, or a letter to: Library of the University of Amsterdam, Secretariat, Singel 425, 1012 WP Amsterdam, The Netherlands. You will be contacted as soon as possible. Download date: 19 May 2020

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UvA-DARE is a service provided by the library of the University of Amsterdam (http://dare.uva.nl)

UvA-DARE (Digital Academic Repository)

Supersymmetric lattice models: Field theory correspondence, integrability, defects anddegeneracies

Fokkema, T.B.

Link to publication

Citation for published version (APA):Fokkema, T. B. (2016). Supersymmetric lattice models: Field theory correspondence, integrability, defects anddegeneracies.

General rightsIt is not permitted to download or to forward/distribute the text or part of it without the consent of the author(s) and/or copyright holder(s),other than for strictly personal, individual use, unless the work is under an open content license (like Creative Commons).

Disclaimer/Complaints regulationsIf you believe that digital publication of certain material infringes any of your rights or (privacy) interests, please let the Library know, statingyour reasons. In case of a legitimate complaint, the Library will make the material inaccessible and/or remove it from the website. Please Askthe Library: https://uba.uva.nl/en/contact, or a letter to: Library of the University of Amsterdam, Secretariat, Singel 425, 1012 WP Amsterdam,The Netherlands. You will be contacted as soon as possible.

Download date: 19 May 2020

Acknowledgements

I would like to thank the people that have been important to me along the roadto this thesis. Thinking back to the years that have past I will mention themchronologically. First I would like to thank Jean-Sebastien Caux, who hired meas a PhD student in september 2011. J.-S. thanks for your confidence in meand giving me the freedom to pursue my own interests. Our discussions ledtogether with Sebas Eliens to a publication which is not part of this thesis. Sebas,thanks a lot for the nice collaboration, we had many insightful discussions andwe learned a lot together. It took us some time to figure out the right questionsand answers and how to interpret the numerical results but it resulted in a verynice publication. At the same time I also learned a lot from discussions withJorn Mossel and Milosz Panfil on the GGE and form factors for the 1D bose gas,thank you for explaining and discussing so many things.

In the summer of 2013 I met Liza Huijse at the low-dimensional quantumcondensed matter workshop in Amsterdam and a few weeks later I joined aresearch project that Liza Huijse and Christian Hagendorf were working on. Thiswork led to our joined paper which is the subject of chapter 3 and 4 of this thesis.Liza, thanks a lot for the many Skype discussions and for making it possible tovisit you at the SITP in Stanford. You explain complex material very well, fromyou I learned about the supersymmetric lattice models that became the subjectof this thesis. You also taught me the basics of conformal field theory and sharedwith me your enthusiasm for these subjects. Christian, thanks for the many hourswe spend discussing, from you I learned very interesting aspects of the Betheansatz which became important in our paper. Thanks for your hospitality inLouvain-la-Neuve.

In the beginning of 2014 I was very interested in the Mk models and conformalfield theory and Kareljan Schoutens and I started to work on a project. Kareljanthen became my PhD supervisor. Kareljan, thanks a lot for suggesting veryinteresting research projects. It has been a great pleasure to work with you. Ourcollaboration went very well and the rest of this thesis (chapters 5, 6 and 7) isbased on our joint results. Kareljan, I am very glad that I have been able to learnso much from you. I also learned a lot from your perseverance and creativity.Many times our discussions lead directly to new ideas and insights which we couldbuilt further on. You have been a great supervisor! Thanks also for carefullyreading the manuscript of this thesis.

Besides the visits that I made to Stanford and Louvain-la-Neuve, I visitedFlorence and Oxford together with Kareljan. I would like to thank Fabian Esslerand Paul Fendley for their hospitality at the Rudolf Peierls Centre in Oxford andAndrea Cappelli for the hospitality at the INFN in Florence. The research in thisthesis also benefited from discussions with Paul Fendley, Ville Lahtenin, JasperStokman, Philippe Corboz and Bernard Nienhuis.

During my PhD I have attended a number of PhD schools. I always enjoyedthese schools a lot because of the opportunity to learn so many new things and

Acknowledgements

meet new people. I would like to thank Rembert Duine and Vincenzo Vitelli forthe organization of the DRSTP PhD schools. Two other schools where I havelearned a lot where the 2014 and 2015 editions of the Lectures on StatisticalField theories at the Galileo Galilei Institute for Theoretical Physics in Florence.Thanks to Andrea Cappelli, Filippo Colomo, Giuseppe Mussardo, Denis Bernardand Gesualdo Delfino for the organization!

I would like to thank my o�ce mates Sebas and Jacopo for the four pleasantyears together in the o�ce. And I would like to thank my other colleagues at theInstitute for Theoretical Physics of the UvA. Especially Bram, Rianne, Rogier,Shanna, Moos, Gyorgy, Ville, Enej, Omar, Davide and Michael. During my PhDI was a teaching assistant for four courses, I would like to thank Bernard Nienhuis,Ari Turner and Theo Nieuwenhuizen for the pleasant collaboration. I wouldalso like to acknowledge the supporting sta↵ of the IoP at the UvA, Yocklang,Anne-Marieke, Natalie, Fatima, Rita and Joost.

Vivian, it has been great to share with you the experiences along the pathtowards a PhD after our master studies in Utrecht. It was nice to share aroom with you at our common schools and conferences. I have been lucky thatthree other good friends, that moved abroad to pursue their PhDs, happenedto live in places that I visited for research. Renee and Thomas, thanks for thegood company during the times I was in Oxford and for letting me stay in yourapartment. Sander, it was great to be able to catch up during my visit to Stanfordand I hope to be able to meet more often again in the future.

Finally, I would like to thank Douwe, Maaike, Marieke, Eveline and Olof forthe support, company and the shared adventures.

187

Contributions to publicationsI would like to emphasise that the published works have been obtained in collab-oration with co-authors. Many hours of discussions and skype sessions have leadto these results. My main contributions to the publications have been

• [1] Relation of the dynamical supersymmetry Q� with Bethe ansatz. Ana-lytical and numerical checks on the action of the dynamical supercharges.Minor contributions to other parts of the article.

• [2] Contributed to all parts of the article and performed all the numericalcomputations.

• [3] Contributed to all parts of the article. Developed algorithm to automatizethe CFT calculations using Mathematica and used this for example to findthe exact two spinon eigenstates of H

2

. Also developed an algorithm whichmade it possible to find the rules which give the spin-content of spin-fullmulti-spinon states.

• [4] Contributed to all parts of this paper.

Bibliography

[1] C. Hagendorf, T. B. Fokkema and L. Huijse, Bethe ansatz solvability andsupersymmetry of the M

2

model of single fermions and pairs, J. Phys. A:Math. Theor. 47 (2014) 485201, arXiv:1408.4403.

[2] T. Fokkema and K. Schoutens, Defects and degeneracies in supersymmetryprotected phases, EPL 111 3 (2015) 30007, arXiv:1504.02421.

[3] T. Fokkema and K. Schoutens, Spinon basis in supersymmetric CFTs,arXiv:1512.07234 (2015).

[4] T. Fokkema and K. Schoutens, Mk models: the field theory connection,work in progress (2015).

[5] T. Fokkema, I. S. Eliens and J.-S. Caux, Split Fermi seas in one-dimensionalBose fluids, Phys. Rev. A 89 3 (2014), arXiv:1401.6857.

[6] P. Fendley, K. Schoutens and J. de Boer, Lattice Models with N = 2Supersymmetry, Phys. Rev. Lett. 90 (2003) 120402, arXiv:hep-th/0210161.

[7] P. Fendley, B. Nienhuis and K. Schoutens, Lattice fermion models withsupersymmetry, J. Phys. A: Math. Gen. 36 (2003) 12399–12424, cond-mat/0307338.

[8] X. Yang and P. Fendley, Non-local spacetime supersymmetry on the lattice,J. Phys. A: Math. Gen. 37 (2004) 8937, arXiv:cond-mat/0404682.

[9] L. Huijse and C. Hagendorf, On the ground states of the M` models, (2015),arXiv:1509.08879.

[10] P. Fendley and C. Hagendorf, Exact and simple results for the XYZ andstrongly interacting fermion chains, J. Phys. A: Math. Theor. 43 (2010)402004.

[11] L. Huijse, N. Moran, J. Vala and K. Schoutens, Exact ground states ofa staggered supersymmetric model for lattice fermions, Phys. Rev. B 84(2011) 115124, arXiv:1103.1368.

[12] M. Beccaria and C. Hagendorf, A staggered fermion chain with supersym-metry on open intervals, J. Phys. A: Math. Theor. 45 (2012) 365201.

[13] L. Huijse and B. Swingle, Area law violations in a supersymmetric model,Phys. Rev. B 87 (2013) 035108, arXiv:1202.2367.

[14] C. Hagendorf and L. Huijse, Bethe ansatz for the M` models of strongly-interacting fermions with supersymmetry, manuscript in preparation. (2015).

[15] A. B. Zamolodchikov and V. A. Fateev, A model factorized S-matrix and anintegrable spin-1 Heisenberg chain, Sov. J. Nucl. Phys. 32 (1981) 298–303.

189

Bibliography

[16] V. A. Fateev, A factorized S-matrix for particles of opposite parities and anintegrable 21-vertex statistical model, Sov. J. Nucl. Phys. 33 (1981) 761–766.

[17] L. Huijse, A supersymmetric model for lattice fermions, PhD thesis,Universiteit van Amsterdam, 2010.

[18] L. Huijse, Detailed analysis of the continuum limit of a supersymmetriclattice model in 1D, J. Stat. Mech. (2011) P04004, arXiv:1102.1700.

[19] P. Fendley and C. Hagendorf, Ground-state properties of a supersymmetricfermion chain, J. Stat. Mech. 1102 (2011) P02014.

[20] L. C. Blom, Supersymmetry on a chain: A handle on strongly interactingfermions, Master’s thesis, Unversiteit van Amsterdam, 2012.

[21] L. Huijse and K. Schoutens, Supersymmetry, lattice fermions, independencecomplexes and cohomology theory, Adv. Theor. Math. Phys. 14.2 (2010)643–694, arXiv:0903.0784.

[22] E. Witten, Constraints on supersymmetry breaking, Nucl. Phys. B 202(1982) 253 – 316.

[23] P. Fendley and K. Schoutens, Exact Results for Strongly CorrelatedFermions in 2+1 Dimensions, Phys. Rev. Lett. 95 4 (2005) 046403, cond-mat/0504595.

[24] P. Fendley, K. Schoutens and H. van Eerten, Hard squares with negativeactivity, J. Phys. A: Math. and Gen. 38 2 (2005) 315, cond-mat/0408497.

[25] H. van Eerten, Extensive ground state entropy in supersymmetric latticemodels, J. Math. Phys. 46 (2005) 123302, cond-mat/0509581.

[26] L. Huijse, J. Halverson, P. Fendley and K. Schoutens, Charge Frustrationand Quantum Criticality for Strongly Correlated Fermions, Phys. Rev. Lett.101 (2008) 146406, arXiv:0804.0174.

[27] J. Jonsson, Certain Homology Cycles of the Independence Complex of Grids,Discrete Comput. Geom. 43 (2010) 927–950.

[28] L. Huijse, D. Mehta, N. Moran, K. Schoutens and J. Vala, Supersymmetriclattice fermions on the triangular lattice: superfrustration and criticality,New. J. Phys. 14 (2012) 073002, arXiv:1112.3314.

[29] B. Bauer, L. Huijse, E. Berg, M. Troyer and K. Schoutens, Supersymmetricmulticritical point in a model of lattice fermions, Phys. Rev. B 87 (2013).

[30] R. Baxter, Exactly solved models in statistical mechanics, London Academic,1982.

190

Bibliography

[31] D. Meidinger and V. Mitev, Dynamic Lattice Supersymmetry in gl(n|m)Spin Chains, arXiv:1312.7021 2013.

[32] K. Hori, S. Katz, A. Klemm, R. Pandharipande, R. Thomas, C. Vafa,R. Vakil and E. Zaslow, Mirror symmetry, Amer. Math. Soc., 2003.

[33] C. Hagendorf, Spin chains with dynamical lattice supersymmetry, J. Stat.Phys. 150 (2013) 609–657.

[34] H. Bethe, Zur theorie der metalle, Zeitschrift fur Physik 71 3-4 (1931)205–226.

[35] N. Crampe, E. Ragoucy and L. Alonzi, Coordinate Bethe ansatz for spin sXXX model, SIGMA 7 (2011) 6, arXiv:1009.0408.

[36] E. T. Whittaker and G. N. Watson, A course of modern analysis, CambridgeUniversity Press, 1927.

[37] R. J. Baxter, Completeness of the Bethe Ansatz for the Six and Eight-VertexModels, J. Stat. Phys. 108 (2002) 1–48.

[38] G. Waterson, Bosonic Construction of an N = 2 Extended SuperconformalTheory in Two-dimensions, Phys. Lett. B 171 (1986) 77.

[39] R. Dijkgraaf, E. P. Verlinde and H. L. Verlinde, c = 1 Conformal FieldTheories on Riemann Surfaces, Commun. Math. Phys. 115 (1988) 649–690.

[40] P. Fendley and K. A. Intriligator, Scattering and thermodynamics offractionally charged supersymmetric solitons, Nucl. Phys. B 372 (1992)533–558, hep-th/9111014.

[41] P. Fendley and K. Intriligator, Scattering and thermodynamics in integrableN = 2 theories, Nucl. Phys. B 380 (1992) 265–290, arXiv:hep-th/9202011.

[42] Z. Bajnok, C. Dunning, L. Palla, G. Takacs and F. Wagner, SUSY sine-Gordon theory as a perturbed conformal field theory and finite size e↵ects,Nucl. Phys. B 679 (2004) 521–544, hep-th/0309120.

[43] A. Hegedus, F. Ravanini and J. Suzuki, Exact finite size spectrum in supersine-Gordon model, Nucl. Phys. B 763 (2007) 330–353.

[44] D. Bernard and A. LeClair, The fractional supersymmetric sine-Gordonmodels, Phys. Lett. B 247 (1990) 309–316.

[45] E. Bergholtz, J. Kailasvuori, E. Wikberg, T. Hansson and A. Karlhede,Pfa�an quantum Hall state made simple: Multiple vacua and domain wallson a thin torus, Phys. Rev. B 74 8 (2006) 081308, cond-mat/0604251.

191

Bibliography

[46] A. Seidel, Abelian and Non-Abelian Hall Liquids and Charge-Density Wave:Quantum Number Fractionalization in One and Two Dimensions, Phys.Rev. Lett. 97 5 (2006), cond-mat/0604465.

[47] E. Ardonne, E. J. Bergholtz, J. Kailasvuori and E. Wikberg, Degeneracy ofnon-abelian quantum Hall states on the torus: Domain walls and conformalfield theory, J. Stat. Mech. 0804 (2008) P04016, arXiv:0802.0675.

[48] J. Lepowski and M. Primc, Structure of standard modules for the a�ne

Lie algebra A(1)

1

, Contemporary Mathematics 46 (1985).

[49] M. Greiter, X. G. Wen and F. Wilczek, Paired hall states, Nucl. Phys. B374 3 (1992) 567–614.

[50] N. Read and E. Rezayi, Beyond paired quantum Hall states: Parafermionsand incompressible states in the first excited Landau level, Phys. Rev. B 59(1999) 8084, cond-mat/9809384.

[51] A. Cappelli, L. S. Georgiev and I. T. Todorov, Parafermion Hall statesfrom coset projections of Abelian conformal theories, Nucl. Phys. B 599 3(2001) 499–530.

[52] G. W. Moore and N. Read, Nonabelions in the fractional quantum Halle↵ect, Nucl. Phys. B 360 (1991) 362–396.

[53] E. Ardonne, N. Read, E. Rezayi and K. Schoutens, NonAbelian spin-singletquantum Hall states: wave functions and quasihole state counting, Nucl.Phys. B 607 (2001) 549–576, cond-mat/0104250.

[54] N. Read and E. Rezayi, Quasiholes and fermionic zero modes of pairedfractional quantum Hall states: The mechanism for non-Abelian statistics,Phys. Rev. B 54 (1996) 16864–16887, cond-mat/9609079.

[55] S. Dasmahapatra, R. Kedem, B. M. McCoy and E. Melzer, Virasorocharacters from Bethe equations for the critical ferromagnetic three statePotts model, J. Stat. Phys. 74 (1994) 239, hep-th/9304150.

[56] A. Berkovich, B. M. McCoy and A. Schilling, Rogers-Schur-Ramanujantype identities for the M(p, p0) minimal models of conformal field theory,Commun. Math. Phys. 191 (1998) 325–395, q-alg/9607020.

[57] P. Bouwknegt and K. Schoutens, Exclusion statistics in conformal fieldtheory - Generalized fermions and spinons for level-1 WZW theories, Nucl.Phys. B 547 (1999) 501–537, hep-th/9810113.

[58] V. P. Yurov and A. B. Zamolodchikov, Truncated conformal space approachto scaling Lee-Yang model, Int. J. Mod. Phys. A5 (1990) 3221–3246.

192

Bibliography

[59] J. Alicea, Y. Oreg, G. Refael, F. von Oppen and M. P. A. Fisher, Non-Abelian statistics and topological quantum information processing in 1Dwire networks, Nat. Phys. 7 5 (2011) 412–417, arXiv:1006.4395.

[60] F. D. M. Haldane, Z. N. C. Ha, J. C. Talstra, D. Bernard and V. Pasquier,Yangian symmetry of integrable quantum chains with long range interactionsand a new description of states in conformal field theory, Phys. Rev. Lett.69 (1992) 2021–2025.

[61] D. Bernard, V. Pasquier and D. Serban, Spinons in conformal field theory,Nucl. Phys.B 428 (1994) 612–628, hep-th/9404050.

[62] P. Bouwknegt, A. W. Ludwig and K. Schoutens, Spinon bases, Yangiansymmetry and fermionic representations of Virasoro characters in conformalfield theory, Phys. Lett. B 338 4 (1994) 448 – 456, hep-th/9406020.

[63] P. Bouwknegt, A. Ludwig and K. Schoutens, A�ne and Yangian symmetriesin SU(2)

1

conformal field theory Spinon bases, Yangian symmetry andfermionic representations of Virasoro characters in conformal field theory,in Proc. of 1994 Summer School in High Energy Physics and Cosmology,E. Gava et al eds. (World Scientific 1995) (1994), hep-th/9412199.

[64] K. Schoutens, Yangian symmetry in conformal field theory, Phys. Lett.B331 (1994) 335–341, hep-th/9401154.

[65] P. Bouwknegt and K. Schoutens, The \SU(n)1

WZW models - Spinondecomposition and yangian structure, Nucl. Phys. B482 (1996) 345–372,hep-th/9607064.

[66] K. Schoutens, Exclusion statistics in conformal field theory spectra, Phys.Rev. Lett. 79 (1997) 2608–2611, cond-mat/9706166.

[67] M. Greiter, Mapping of Parent Hamiltonians: From Abelian and non-Abelian Quantum Hall States to Exact Models of Critical Spin Chains,Springer Tracts in Modern Physics Vol. 244 (2011), arXiv:1109.6104.

[68] B. Paredes, Non-Abelian fractional quantum Hall states for hard-core bosonsin one dimension, Phys. Rev. B 85 19 (2012) 195150.

[69] A. E. B. Nielsen, J. I. Cirac and G. Sierra, Quantum spin Hamiltoni-ans for the SU(2)k WZW model, J. Stat. Mech. 1111 (2011) P11014,arXiv:1109.5470.

[70] H.-H. Tu, A. E. B. Nielsen, J. I. Cirac and G. Sierra, Lattice Laughlin statesof bosons and fermions at filling fractions 1/q, New J. Phys. 16 (2014)033025, arXiv:1311.3958.

193

Bibliography

[71] I. Glasser, J. I. Cirac, G. Sierra and A. E. B. Nielsen, Exact parentHamiltonians of bosonic and fermionic Moore–Read states on lattices andlocal models, New J. Phys. 17 8 (2015) 082001.

[72] R. Thomale, S. Rachel, P. Schmitteckert and M. Greiter, A Family ofspin-S chain representations of SU(2)k Wess-Zumino-Witten models, Phys.Rev. B85 (2012) 195149, arXiv:1110.5956.

[73] P. Bouwknegt, A. W. W. Ludwig and K. Schoutens, Spinon basis forhigher level SU(2) WZW models, Phys. Lett.B 359 (1995) 304–312, hep-th/9412108.

[74] V. Drinfeld, Quantum Groups, Proc. ICM Berkeley (1986).

[75] V. A. Fateev and A. B. Zamolodchikov, Parafermionic Currents in theTwo-Dimensional Conformal Quantum Field Theory and Selfdual CriticalPoints in Z(n) Invariant Statistical Systems, Sov. Phys. JETP 62 (1985)215–225.

[76] K. Schoutens, Exclusion Statistics for Non-Abelian Quantum Hall States,Phys. Rev. Lett. 81 (1998) 1929–1932.

[77] E. Ardonne and K. Schoutens, New Class of Non-Abelian Spin-SingletQuantum Hall States, Phys. Rev. Lett. 82 25 (1999) 5096–5099, cond-mat/9811352.

[78] R. Santachiara and K. Schoutens, Supersymmetric model of spin-1/2fermions on a chain, J. Phys. A: Math. Gen. 38 24 (2005) 5425, cond-mat/0503354.

[79] R. I. Nepomechie, Supersymmetry in the boundary tricritical Ising fieldtheory, Int. J. Mod. Phys. A 17 (2002) 3809, hep-th/0203123.

[80] L. Chim, Boundary S matrix for the tricritical Ising model, Int. J. Mod.Phys. A. 11 (1996) 4491–4512, hep-th/9510008.

[81] C. Ahn and W. M. Koo, Exact boundary S matrices of the supersymmetricSine-Gordon theory on a half line, J. Phys. A. 29 (1996) 5845–5854, hep-th/9509056.

[82] P. D. Francesco, P. Mathieu and D. Senechal, Conformal Field Theory,Graduate Texts in Contemporary Physics, Springer, 1997.

[83] P. Ginsparg, Applied Conformal Field Theory, Fields, Strings and CriticalPhenomena, (Les Houches, Session XLIX, 1988) ed. by E. Brezin and J.Zinn Justin, 1989 (1991), hep-th/9108028.

[84] G. Mussardo, Statistical Field Theory: An Introduction to Exactly SolvedModels in Statistical Physics, Oxford Graduate Texts, OUP Oxford, 2009.

194

Bibliography

[85] F. A. Bais, P. Bouwknegt, M. Surridge and K. Schoutens, Extensions ofthe Virasoro Algebra Constructed from Kac-Moody Algebras Using HigherOrder Casimir Invariants, Nucl. Phys. B304 (1988) 348–370.

[86] A. A. Belavin, A. M. Polyakov and A. B. Zamolodchikov, Infinite ConformalSymmetry in Two-Dimensional Quantum Field Theory, Nucl. Phys. B 241(1984) 333–380.

[87] W. Lerche, C. Vafa and N. P. Warner, Chiral rings in N = 2 superconformalfield theories, Nucl. Phys. B 324 (1989) 427–474.

[88] N. P. Warner, N = 2 supersymmetric integrable models and topological fieldtheories, in Trieste Summer School on High-energy Physics and CosmologyTrieste, Italy, June 15-August 14, 1992, 1993, hep-th/9301088.

[89] L. Dixon, P. Ginsparg and J. Harvey, c = 1 Superconformal Field Theory,Nucl. Phys. B 306 3 (1988) 470 – 496.

[90] A. Schwimmer and N. Seiberg, Comments on the N = 2, 3, 4 superconformalalgebras in two dimensions, Phys. Lett. B 184 2–3 (1987) 191 – 196.

[91] L. J. Dixon, D. Friedan, E. J. Martinec and S. H. Shenker, The ConformalField Theory of Orbifolds, Nucl. Phys.B 282 (1987) 13–73.

[92] D. Friedan, Z.-a. Qiu and S. H. Shenker, Superconformal Invariance inTwo-Dimensions and the Tricritical Ising Model, Phys. Lett. B 151 (1985)37–43.

[93] S. Ghoshal and A. B. Zamolodchikov, Boundary S matrix and boundarystate in two-dimensional integrable quantum field theory, Int. J. Mod. Phys.A. 9 (1994) 3841–3886, hep-th/9306002.

[94] P. Baseilhac and K. Koizumi, N = 2 boundary supersymmetry in integrablemodels and perturbed boundary conformal field theory, Nucl. Phys. B. 669(2003) 417–434, hep-th/0304120.

[95] E. Witten and D. I. Olive, Supersymmetry Algebras That Include TopologicalCharges, Phys. Lett. B 78 (1978) 97.

[96] K. Schoutens, Supersymmetry and Factorizable Scattering, Nucl. Phys. B344 (1990) 665–695.

[97] P. Fendley, S. Mathur, C. Vafa and N. Warner, Integrable Deformationsand Scattering Matrices for the N = 2 Supersymmetric Discrete Series,Phys. Lett. B 243 (1990) 257–264.

[98] N. P. Warner, Supersymmetry in boundary integrable models, Nucl. Phys.B 450 (1995) 663–694, hep-th/9506064.

195

Bibliography

[99] A. Zamolodchikov, Fractional spin integrals of motion in perturbed confor-mal field theory, (1989).

[100] C. Vafa and N. P. Warner, Catastrophes and the Classification of ConformalTheories, Phys. Lett. B 218 (1989) 51.

[101] P. Fendley, W. Lerche, S. Mathur and N. Warner, N=2 supersymmetricintegrable models from a�ne toda theories, Nucl. Phys. B 348 (1991) 66–88.

[102] R. Dijkgraaf, H. Verlinde and E. Verlinde, Topological strings in d<1, Nucl.Phys. B 352 1 (1991) 59 – 86.

196