| Home > Publications database > Finite-Volume Energy Spectrum, Fractionalized Strings, and Low-Energy Effective Field Theory for the Quantum Dimer Model on the Square Lattice > print |
| 001 | 292470 | ||
| 005 | 20211110132848.0 | ||
| 024 | 7 | _ | |a arXiv:1511.00881 |2 arXiv |
| 024 | 7 | _ | |a altmetric:4721173 |2 altmetric |
| 024 | 7 | _ | |a inspire:1402962 |2 inspire |
| 037 | _ | _ | |a PUBDB-2015-06120 |
| 088 | 1 | _ | |a arXiv:1511.00881 |
| 088 | _ | _ | |a arXiv:1511.00881 |2 arXiv |
| 100 | 1 | _ | |a Banerjee, Debasish |0 P:(DE-H253)PIP1024140 |b 0 |e Corresponding author |u desy |
| 245 | _ | _ | |a Finite-Volume Energy Spectrum, Fractionalized Strings, and Low-Energy Effective Field Theory for the Quantum Dimer Model on the Square Lattice |
| 260 | _ | _ | |c 2015 |
| 300 | _ | _ | |a 35 p. |
| 336 | 7 | _ | |a report |2 DRIVER |
| 336 | 7 | _ | |a REPORT |2 ORCID |
| 336 | 7 | _ | |a Report |0 10 |2 EndNote |
| 336 | 7 | _ | |a Output Types/Report |2 DataCite |
| 336 | 7 | _ | |a Report |b report |m report |0 PUB:(DE-HGF)29 |s 1480949728_1456 |2 PUB:(DE-HGF) |
| 336 | 7 | _ | |a TECHREPORT |2 BibTeX |
| 520 | _ | _ | |a We present detailed analytic calculations of finite-volume energy spectra, mean field theory, as well as a systematic low-energy effective field theory for the square lattice quantum dimer model. The analytic considerations explain why a string connecting two external static charges in the confining columnar phase fractionalizes into eight distinct strands with electric flux $\frac{1}{4}$. An emergent approximate spontaneously broken $SO(2)$ symmetry gives rise to a pseudo-Goldstone boson. Remarkably, this soft phonon-like excitation, which is massless at the Rokhsar-Kivelson (RK) point, exists far beyond this point. The Goldstone physics is captured by a systematic low-energy effective field theory. We determine its low-energy parameters by matching the analytic effective field theory with exact diagonalization results and Monte Carlo data. This confirms that the model exists in the columnar (and not in a plaquette or mixed) phase all the way to the RK point. |
| 536 | _ | _ | |0 G:(DE-HGF)POF3-611 |c POF3-611 |f POF III |x 0 |a 611 - Fundamental Particles and Forces (POF3-611) |
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| 700 | 1 | _ | |a B'ogli, M. |0 P:(DE-HGF)0 |b 1 |
| 700 | 1 | _ | |a Hofmann, C. P. |0 P:(DE-HGF)0 |b 2 |
| 700 | 1 | _ | |a Jiang, F. -J. |0 P:(DE-HGF)0 |b 3 |
| 700 | 1 | _ | |a Widmer, P. |0 P:(DE-HGF)0 |b 4 |
| 700 | 1 | _ | |a Wiese, U. -J. |0 P:(DE-HGF)0 |b 5 |
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| 910 | 1 | _ | |a Deutsches Elektronen-Synchrotron |0 I:(DE-588b)2008985-5 |k DESY |b 0 |6 P:(DE-H253)PIP1024140 |
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| 914 | 1 | _ | |y 2015 |
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