Integrable lambda models and Chern-Simons theories

Abstract In this note we reveal a connection between the phase space of lambda models on %$ {S}^1\times \mathbb{R} %$ and the phase space of double Chern-Simons theories on %$ D\times \mathbb{R} %$ and explain in the process the origin of the non-ultralocality of the Maillet bracket, which emerges a...
Ausführliche Beschreibung

Gespeichert in:

Autor*in:	Schmidtt, David M. [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2017

Schlagwörter:	Chern-Simons Theories Integrable Field Theories Sigma Models Integrable Hierarchies

Anmerkung:	© The Author(s) 2017

Übergeordnetes Werk:	Enthalten in: Journal of high energy physics - Berlin : Springer, 1997, 2017(2017), 5 vom: 03. Mai
Übergeordnetes Werk:	volume:2017 ; year:2017 ; number:5 ; day:03 ; month:05

Links:	Volltext

DOI / URN:	10.1007/JHEP05(2017)012

Katalog-ID:	SPR030534593

Internformat


LEADER	01000caa a22002652 4500
001	SPR030534593
003	DE-627
005	20230331092229.0
007	cr uuu---uuuuu
008	201007s2017 xx \|\|\|\|\|o 00\| \|\|eng c
024	7		\|a 10.1007/JHEP05(2017)012 \|2 doi
035			\|a (DE-627)SPR030534593
035			\|a (SPR)JHEP05(2017)012-e
040			\|a DE-627 \|b ger \|c DE-627 \|e rakwb
041			\|a eng
100	1		\|a Schmidtt, David M. \|e verfasserin \|4 aut
245	1	0	\|a Integrable lambda models and Chern-Simons theories
264		1	\|c 2017
336			\|a Text \|b txt \|2 rdacontent
337			\|a Computermedien \|b c \|2 rdamedia
338			\|a Online-Ressource \|b cr \|2 rdacarrier
500			\|a © The Author(s) 2017
520			\|a Abstract In this note we reveal a connection between the phase space of lambda models on %$ {S}^1\times \mathbb{R} %$ and the phase space of double Chern-Simons theories on %$ D\times \mathbb{R} %$ and explain in the process the origin of the non-ultralocality of the Maillet bracket, which emerges as a boundary algebra. In particular, this means that the (classical) AdS5 × S5 lambda model can be understood as a double Chern-Simons theory defined on the Lie superalgebra %$ \mathfrak{p}\mathfrak{s}\mathfrak{u}\left(2,2\Big\|4\right) %$ after a proper dependence of the spectral parameter is introduced. This offers a possibility for avoiding the use of the problematic non-ultralocal Poisson algebras that preclude the introduction of lattice regularizations and the application of the QISM to string sigma models. The utility of the equivalence at the quantum level is, however, still to be explored.
650		4	\|a Chern-Simons Theories \|7 (dpeaa)DE-He213
650		4	\|a Integrable Field Theories \|7 (dpeaa)DE-He213
650		4	\|a Sigma Models \|7 (dpeaa)DE-He213
650		4	\|a Integrable Hierarchies \|7 (dpeaa)DE-He213
773	0	8	\|i Enthalten in \|t Journal of high energy physics \|d Berlin : Springer, 1997 \|g 2017(2017), 5 vom: 03. Mai \|w (DE-627)320910571 \|w (DE-600)2027350-2 \|x 1029-8479 \|7 nnns
773	1	8	\|g volume:2017 \|g year:2017 \|g number:5 \|g day:03 \|g month:05
856	4	0	\|u https://dx.doi.org/10.1007/JHEP05(2017)012 \|z kostenfrei \|3 Volltext
912			\|a GBV_USEFLAG_A
912			\|a SYSFLAG_A
912			\|a GBV_SPRINGER
912			\|a GBV_ILN_20
912			\|a GBV_ILN_22
912			\|a GBV_ILN_23
912			\|a GBV_ILN_24
912			\|a GBV_ILN_31
912			\|a GBV_ILN_39
912			\|a GBV_ILN_40
912			\|a GBV_ILN_60
912			\|a GBV_ILN_62
912			\|a GBV_ILN_63
912			\|a GBV_ILN_65
912			\|a GBV_ILN_69
912			\|a GBV_ILN_70
912			\|a GBV_ILN_73
912			\|a GBV_ILN_95
912			\|a GBV_ILN_105
912			\|a GBV_ILN_110
912			\|a GBV_ILN_151
912			\|a GBV_ILN_161
912			\|a GBV_ILN_170
912			\|a GBV_ILN_213
912			\|a GBV_ILN_230
912			\|a GBV_ILN_285
912			\|a GBV_ILN_293
912			\|a GBV_ILN_370
912			\|a GBV_ILN_602
912			\|a GBV_ILN_2014
912			\|a GBV_ILN_2020
912			\|a GBV_ILN_4012
912			\|a GBV_ILN_4037
912			\|a GBV_ILN_4112
912			\|a GBV_ILN_4125
912			\|a GBV_ILN_4126
912			\|a GBV_ILN_4249
912			\|a GBV_ILN_4305
912			\|a GBV_ILN_4306
912			\|a GBV_ILN_4307
912			\|a GBV_ILN_4313
912			\|a GBV_ILN_4322
912			\|a GBV_ILN_4323
912			\|a GBV_ILN_4324
912			\|a GBV_ILN_4325
912			\|a GBV_ILN_4335
912			\|a GBV_ILN_4338
912			\|a GBV_ILN_4367
912			\|a GBV_ILN_4700
951			\|a AR
952			\|d 2017 \|j 2017 \|e 5 \|b 03 \|c 05

Indexfelder

author_variant	d m s dm dms
matchkey_str	article:10298479:2017----::nerbeabaoesnceni
hierarchy_sort_str	2017
publishDate	2017
allfields	10.1007/JHEP05(2017)012 doi (DE-627)SPR030534593 (SPR)JHEP05(2017)012-e DE-627 ger DE-627 rakwb eng Schmidtt, David M. verfasserin aut Integrable lambda models and Chern-Simons theories 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s) 2017 Abstract In this note we reveal a connection between the phase space of lambda models on %$ {S}^1\times \mathbb{R} %$ and the phase space of double Chern-Simons theories on %$ D\times \mathbb{R} %$ and explain in the process the origin of the non-ultralocality of the Maillet bracket, which emerges as a boundary algebra. In particular, this means that the (classical) AdS5 × S5 lambda model can be understood as a double Chern-Simons theory defined on the Lie superalgebra %$ \mathfrak{p}\mathfrak{s}\mathfrak{u}\left(2,2\Big\|4\right) %$ after a proper dependence of the spectral parameter is introduced. This offers a possibility for avoiding the use of the problematic non-ultralocal Poisson algebras that preclude the introduction of lattice regularizations and the application of the QISM to string sigma models. The utility of the equivalence at the quantum level is, however, still to be explored. Chern-Simons Theories (dpeaa)DE-He213 Integrable Field Theories (dpeaa)DE-He213 Sigma Models (dpeaa)DE-He213 Integrable Hierarchies (dpeaa)DE-He213 Enthalten in Journal of high energy physics Berlin : Springer, 1997 2017(2017), 5 vom: 03. Mai (DE-627)320910571 (DE-600)2027350-2 1029-8479 nnns volume:2017 year:2017 number:5 day:03 month:05 https://dx.doi.org/10.1007/JHEP05(2017)012 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_2020 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 2017 2017 5 03 05
spelling	10.1007/JHEP05(2017)012 doi (DE-627)SPR030534593 (SPR)JHEP05(2017)012-e DE-627 ger DE-627 rakwb eng Schmidtt, David M. verfasserin aut Integrable lambda models and Chern-Simons theories 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s) 2017 Abstract In this note we reveal a connection between the phase space of lambda models on %$ {S}^1\times \mathbb{R} %$ and the phase space of double Chern-Simons theories on %$ D\times \mathbb{R} %$ and explain in the process the origin of the non-ultralocality of the Maillet bracket, which emerges as a boundary algebra. In particular, this means that the (classical) AdS5 × S5 lambda model can be understood as a double Chern-Simons theory defined on the Lie superalgebra %$ \mathfrak{p}\mathfrak{s}\mathfrak{u}\left(2,2\Big\|4\right) %$ after a proper dependence of the spectral parameter is introduced. This offers a possibility for avoiding the use of the problematic non-ultralocal Poisson algebras that preclude the introduction of lattice regularizations and the application of the QISM to string sigma models. The utility of the equivalence at the quantum level is, however, still to be explored. Chern-Simons Theories (dpeaa)DE-He213 Integrable Field Theories (dpeaa)DE-He213 Sigma Models (dpeaa)DE-He213 Integrable Hierarchies (dpeaa)DE-He213 Enthalten in Journal of high energy physics Berlin : Springer, 1997 2017(2017), 5 vom: 03. Mai (DE-627)320910571 (DE-600)2027350-2 1029-8479 nnns volume:2017 year:2017 number:5 day:03 month:05 https://dx.doi.org/10.1007/JHEP05(2017)012 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_2020 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 2017 2017 5 03 05
allfields_unstemmed	10.1007/JHEP05(2017)012 doi (DE-627)SPR030534593 (SPR)JHEP05(2017)012-e DE-627 ger DE-627 rakwb eng Schmidtt, David M. verfasserin aut Integrable lambda models and Chern-Simons theories 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s) 2017 Abstract In this note we reveal a connection between the phase space of lambda models on %$ {S}^1\times \mathbb{R} %$ and the phase space of double Chern-Simons theories on %$ D\times \mathbb{R} %$ and explain in the process the origin of the non-ultralocality of the Maillet bracket, which emerges as a boundary algebra. In particular, this means that the (classical) AdS5 × S5 lambda model can be understood as a double Chern-Simons theory defined on the Lie superalgebra %$ \mathfrak{p}\mathfrak{s}\mathfrak{u}\left(2,2\Big\|4\right) %$ after a proper dependence of the spectral parameter is introduced. This offers a possibility for avoiding the use of the problematic non-ultralocal Poisson algebras that preclude the introduction of lattice regularizations and the application of the QISM to string sigma models. The utility of the equivalence at the quantum level is, however, still to be explored. Chern-Simons Theories (dpeaa)DE-He213 Integrable Field Theories (dpeaa)DE-He213 Sigma Models (dpeaa)DE-He213 Integrable Hierarchies (dpeaa)DE-He213 Enthalten in Journal of high energy physics Berlin : Springer, 1997 2017(2017), 5 vom: 03. Mai (DE-627)320910571 (DE-600)2027350-2 1029-8479 nnns volume:2017 year:2017 number:5 day:03 month:05 https://dx.doi.org/10.1007/JHEP05(2017)012 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_2020 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 2017 2017 5 03 05
allfieldsGer	10.1007/JHEP05(2017)012 doi (DE-627)SPR030534593 (SPR)JHEP05(2017)012-e DE-627 ger DE-627 rakwb eng Schmidtt, David M. verfasserin aut Integrable lambda models and Chern-Simons theories 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s) 2017 Abstract In this note we reveal a connection between the phase space of lambda models on %$ {S}^1\times \mathbb{R} %$ and the phase space of double Chern-Simons theories on %$ D\times \mathbb{R} %$ and explain in the process the origin of the non-ultralocality of the Maillet bracket, which emerges as a boundary algebra. In particular, this means that the (classical) AdS5 × S5 lambda model can be understood as a double Chern-Simons theory defined on the Lie superalgebra %$ \mathfrak{p}\mathfrak{s}\mathfrak{u}\left(2,2\Big\|4\right) %$ after a proper dependence of the spectral parameter is introduced. This offers a possibility for avoiding the use of the problematic non-ultralocal Poisson algebras that preclude the introduction of lattice regularizations and the application of the QISM to string sigma models. The utility of the equivalence at the quantum level is, however, still to be explored. Chern-Simons Theories (dpeaa)DE-He213 Integrable Field Theories (dpeaa)DE-He213 Sigma Models (dpeaa)DE-He213 Integrable Hierarchies (dpeaa)DE-He213 Enthalten in Journal of high energy physics Berlin : Springer, 1997 2017(2017), 5 vom: 03. Mai (DE-627)320910571 (DE-600)2027350-2 1029-8479 nnns volume:2017 year:2017 number:5 day:03 month:05 https://dx.doi.org/10.1007/JHEP05(2017)012 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_2020 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 2017 2017 5 03 05
allfieldsSound	10.1007/JHEP05(2017)012 doi (DE-627)SPR030534593 (SPR)JHEP05(2017)012-e DE-627 ger DE-627 rakwb eng Schmidtt, David M. verfasserin aut Integrable lambda models and Chern-Simons theories 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s) 2017 Abstract In this note we reveal a connection between the phase space of lambda models on %$ {S}^1\times \mathbb{R} %$ and the phase space of double Chern-Simons theories on %$ D\times \mathbb{R} %$ and explain in the process the origin of the non-ultralocality of the Maillet bracket, which emerges as a boundary algebra. In particular, this means that the (classical) AdS5 × S5 lambda model can be understood as a double Chern-Simons theory defined on the Lie superalgebra %$ \mathfrak{p}\mathfrak{s}\mathfrak{u}\left(2,2\Big\|4\right) %$ after a proper dependence of the spectral parameter is introduced. This offers a possibility for avoiding the use of the problematic non-ultralocal Poisson algebras that preclude the introduction of lattice regularizations and the application of the QISM to string sigma models. The utility of the equivalence at the quantum level is, however, still to be explored. Chern-Simons Theories (dpeaa)DE-He213 Integrable Field Theories (dpeaa)DE-He213 Sigma Models (dpeaa)DE-He213 Integrable Hierarchies (dpeaa)DE-He213 Enthalten in Journal of high energy physics Berlin : Springer, 1997 2017(2017), 5 vom: 03. Mai (DE-627)320910571 (DE-600)2027350-2 1029-8479 nnns volume:2017 year:2017 number:5 day:03 month:05 https://dx.doi.org/10.1007/JHEP05(2017)012 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_2020 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 2017 2017 5 03 05
language	English
source	Enthalten in Journal of high energy physics 2017(2017), 5 vom: 03. Mai volume:2017 year:2017 number:5 day:03 month:05
sourceStr	Enthalten in Journal of high energy physics 2017(2017), 5 vom: 03. Mai volume:2017 year:2017 number:5 day:03 month:05
format_phy_str_mv	Article
institution	findex.gbv.de
topic_facet	Chern-Simons Theories Integrable Field Theories Sigma Models Integrable Hierarchies
isfreeaccess_bool	true
container_title	Journal of high energy physics
authorswithroles_txt_mv	Schmidtt, David M. @@aut@@
publishDateDaySort_date	2017-05-03T00:00:00Z
hierarchy_top_id	320910571
id	SPR030534593
language_de	englisch
fullrecord	<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">SPR030534593</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230331092229.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">201007s2017 xx \|\|\|\|\|o 00\| \|\|eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/JHEP05(2017)012</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR030534593</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)JHEP05(2017)012-e</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Schmidtt, David M.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Integrable lambda models and Chern-Simons theories</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2017</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© The Author(s) 2017</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract In this note we reveal a connection between the phase space of lambda models on %$ {S}^1\times \mathbb{R} %$ and the phase space of double Chern-Simons theories on %$ D\times \mathbb{R} %$ and explain in the process the origin of the non-ultralocality of the Maillet bracket, which emerges as a boundary algebra. In particular, this means that the (classical) AdS5 × S5 lambda model can be understood as a double Chern-Simons theory defined on the Lie superalgebra %$ \mathfrak{p}\mathfrak{s}\mathfrak{u}\left(2,2\Big\|4\right) %$ after a proper dependence of the spectral parameter is introduced. This offers a possibility for avoiding the use of the problematic non-ultralocal Poisson algebras that preclude the introduction of lattice regularizations and the application of the QISM to string sigma models. The utility of the equivalence at the quantum level is, however, still to be explored.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Chern-Simons Theories</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Integrable Field Theories</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Sigma Models</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Integrable Hierarchies</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Journal of high energy physics</subfield><subfield code="d">Berlin : Springer, 1997</subfield><subfield code="g">2017(2017), 5 vom: 03. Mai</subfield><subfield code="w">(DE-627)320910571</subfield><subfield code="w">(DE-600)2027350-2</subfield><subfield code="x">1029-8479</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:2017</subfield><subfield code="g">year:2017</subfield><subfield code="g">number:5</subfield><subfield code="g">day:03</subfield><subfield code="g">month:05</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://dx.doi.org/10.1007/JHEP05(2017)012</subfield><subfield code="z">kostenfrei</subfield><subfield code="3">Volltext</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_SPRINGER</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_20</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_22</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_23</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_24</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_31</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_39</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_40</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_60</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_62</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_63</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_65</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_69</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_73</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_95</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_105</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_110</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_151</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_161</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_170</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_213</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_230</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_285</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_293</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_370</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_602</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2014</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2020</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4012</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4037</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4112</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4125</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4126</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4249</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4305</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4306</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4307</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4313</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4322</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4323</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4324</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4325</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4335</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4338</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4367</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4700</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">2017</subfield><subfield code="j">2017</subfield><subfield code="e">5</subfield><subfield code="b">03</subfield><subfield code="c">05</subfield></datafield></record></collection>
author	Schmidtt, David M.
spellingShingle	Schmidtt, David M. misc Chern-Simons Theories misc Integrable Field Theories misc Sigma Models misc Integrable Hierarchies Integrable lambda models and Chern-Simons theories
authorStr	Schmidtt, David M.
ppnlink_with_tag_str_mv	@@773@@(DE-627)320910571
format	electronic Article
delete_txt_mv	keep
author_role	aut
collection	springer
remote_str	true
illustrated	Not Illustrated
issn	1029-8479
topic_title	Integrable lambda models and Chern-Simons theories Chern-Simons Theories (dpeaa)DE-He213 Integrable Field Theories (dpeaa)DE-He213 Sigma Models (dpeaa)DE-He213 Integrable Hierarchies (dpeaa)DE-He213
topic	misc Chern-Simons Theories misc Integrable Field Theories misc Sigma Models misc Integrable Hierarchies
topic_unstemmed	misc Chern-Simons Theories misc Integrable Field Theories misc Sigma Models misc Integrable Hierarchies
topic_browse	misc Chern-Simons Theories misc Integrable Field Theories misc Sigma Models misc Integrable Hierarchies
format_facet	Elektronische Aufsätze Aufsätze Elektronische Ressource
format_main_str_mv	Text Zeitschrift/Artikel
carriertype_str_mv	cr
hierarchy_parent_title	Journal of high energy physics
hierarchy_parent_id	320910571
hierarchy_top_title	Journal of high energy physics
isfreeaccess_txt	true
familylinks_str_mv	(DE-627)320910571 (DE-600)2027350-2
title	Integrable lambda models and Chern-Simons theories
ctrlnum	(DE-627)SPR030534593 (SPR)JHEP05(2017)012-e
title_full	Integrable lambda models and Chern-Simons theories
author_sort	Schmidtt, David M.
journal	Journal of high energy physics
journalStr	Journal of high energy physics
lang_code	eng
isOA_bool	true
recordtype	marc
publishDateSort	2017
contenttype_str_mv	txt
author_browse	Schmidtt, David M.
container_volume	2017
format_se	Elektronische Aufsätze
author-letter	Schmidtt, David M.
doi_str_mv	10.1007/JHEP05(2017)012
title_sort	integrable lambda models and chern-simons theories
title_auth	Integrable lambda models and Chern-Simons theories
abstract	Abstract In this note we reveal a connection between the phase space of lambda models on %$ {S}^1\times \mathbb{R} %$ and the phase space of double Chern-Simons theories on %$ D\times \mathbb{R} %$ and explain in the process the origin of the non-ultralocality of the Maillet bracket, which emerges as a boundary algebra. In particular, this means that the (classical) AdS5 × S5 lambda model can be understood as a double Chern-Simons theory defined on the Lie superalgebra %$ \mathfrak{p}\mathfrak{s}\mathfrak{u}\left(2,2\Big\|4\right) %$ after a proper dependence of the spectral parameter is introduced. This offers a possibility for avoiding the use of the problematic non-ultralocal Poisson algebras that preclude the introduction of lattice regularizations and the application of the QISM to string sigma models. The utility of the equivalence at the quantum level is, however, still to be explored. © The Author(s) 2017
abstractGer	Abstract In this note we reveal a connection between the phase space of lambda models on %$ {S}^1\times \mathbb{R} %$ and the phase space of double Chern-Simons theories on %$ D\times \mathbb{R} %$ and explain in the process the origin of the non-ultralocality of the Maillet bracket, which emerges as a boundary algebra. In particular, this means that the (classical) AdS5 × S5 lambda model can be understood as a double Chern-Simons theory defined on the Lie superalgebra %$ \mathfrak{p}\mathfrak{s}\mathfrak{u}\left(2,2\Big\|4\right) %$ after a proper dependence of the spectral parameter is introduced. This offers a possibility for avoiding the use of the problematic non-ultralocal Poisson algebras that preclude the introduction of lattice regularizations and the application of the QISM to string sigma models. The utility of the equivalence at the quantum level is, however, still to be explored. © The Author(s) 2017
abstract_unstemmed	Abstract In this note we reveal a connection between the phase space of lambda models on %$ {S}^1\times \mathbb{R} %$ and the phase space of double Chern-Simons theories on %$ D\times \mathbb{R} %$ and explain in the process the origin of the non-ultralocality of the Maillet bracket, which emerges as a boundary algebra. In particular, this means that the (classical) AdS5 × S5 lambda model can be understood as a double Chern-Simons theory defined on the Lie superalgebra %$ \mathfrak{p}\mathfrak{s}\mathfrak{u}\left(2,2\Big\|4\right) %$ after a proper dependence of the spectral parameter is introduced. This offers a possibility for avoiding the use of the problematic non-ultralocal Poisson algebras that preclude the introduction of lattice regularizations and the application of the QISM to string sigma models. The utility of the equivalence at the quantum level is, however, still to be explored. © The Author(s) 2017
collection_details	GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_2020 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700
container_issue	5
title_short	Integrable lambda models and Chern-Simons theories
url	https://dx.doi.org/10.1007/JHEP05(2017)012
remote_bool	true
ppnlink	320910571
mediatype_str_mv	c
isOA_txt	true
hochschulschrift_bool	false
doi_str	10.1007/JHEP05(2017)012
up_date	2024-07-03T17:59:24.576Z
_version_	1803581720705892352
fullrecord_marcxml	<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">SPR030534593</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230331092229.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">201007s2017 xx \|\|\|\|\|o 00\| \|\|eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/JHEP05(2017)012</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR030534593</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)JHEP05(2017)012-e</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Schmidtt, David M.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Integrable lambda models and Chern-Simons theories</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2017</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© The Author(s) 2017</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract In this note we reveal a connection between the phase space of lambda models on %$ {S}^1\times \mathbb{R} %$ and the phase space of double Chern-Simons theories on %$ D\times \mathbb{R} %$ and explain in the process the origin of the non-ultralocality of the Maillet bracket, which emerges as a boundary algebra. In particular, this means that the (classical) AdS5 × S5 lambda model can be understood as a double Chern-Simons theory defined on the Lie superalgebra %$ \mathfrak{p}\mathfrak{s}\mathfrak{u}\left(2,2\Big\|4\right) %$ after a proper dependence of the spectral parameter is introduced. This offers a possibility for avoiding the use of the problematic non-ultralocal Poisson algebras that preclude the introduction of lattice regularizations and the application of the QISM to string sigma models. The utility of the equivalence at the quantum level is, however, still to be explored.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Chern-Simons Theories</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Integrable Field Theories</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Sigma Models</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Integrable Hierarchies</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Journal of high energy physics</subfield><subfield code="d">Berlin : Springer, 1997</subfield><subfield code="g">2017(2017), 5 vom: 03. Mai</subfield><subfield code="w">(DE-627)320910571</subfield><subfield code="w">(DE-600)2027350-2</subfield><subfield code="x">1029-8479</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:2017</subfield><subfield code="g">year:2017</subfield><subfield code="g">number:5</subfield><subfield code="g">day:03</subfield><subfield code="g">month:05</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://dx.doi.org/10.1007/JHEP05(2017)012</subfield><subfield code="z">kostenfrei</subfield><subfield code="3">Volltext</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_SPRINGER</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_20</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_22</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_23</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_24</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_31</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_39</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_40</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_60</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_62</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_63</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_65</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_69</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_73</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_95</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_105</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_110</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_151</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_161</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_170</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_213</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_230</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_285</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_293</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_370</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_602</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2014</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2020</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4012</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4037</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4112</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4125</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4126</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4249</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4305</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4306</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4307</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4313</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4322</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4323</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4324</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4325</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4335</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4338</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4367</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4700</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">2017</subfield><subfield code="j">2017</subfield><subfield code="e">5</subfield><subfield code="b">03</subfield><subfield code="c">05</subfield></datafield></record></collection>
score	7.3989944

Nicht das Richtige dabei?

Schreiben Sie uns!

Integrable lambda models and Chern-Simons theories

Nicht das Richtige dabei?

Zugang & Verfügbarkeit

Vorhandene Bände

Nicht das Richtige dabei?