Polymer Optical Fibre (POF) Bragg gratings for Nuclear Waste Repositories. Broadway, C., Kinet, D., Theodosiou, A., Kalli, K., Caucheteur, C., & Mégret, P. In 08 April 2019. Submitted to Physics Letters Babstract bibtex The Lambda(b) differential production cross section and the cross section ratio anti-Lambda(b)/Lambda(b) are measured as functions of transverse momentum pt(Lambda(b)) and rapidity abs(y(Lambda(b))) in pp collisions at sqrt(s) = 7 TeV using data collected by the CMS experiment at the LHC. The measurements are based on Lambda(b) decays reconstructed in the exclusive final state J/Psi Lambda, with the subsequent decays J/Psi to an opposite-sign muon pair and Lambda to proton pion, using a data sample corresponding to an integrated luminosity of 1.9 inverse femtobarns. The product of the cross section times the branching ratio for Lambda(b) to J/Psi Lambda versus pt(Lambda(b)) falls faster than that of b mesons. The measured value of the cross section times the branching ratio for pt(Lambda(b)) > 10 GeV and abs(y(Lambda(b))) < 2.0 is 1.06 +/- 0.06 +/- 0.12 nb, and the integrated cross section ratio for anti-Lambda(b)/Lambda(b) is 1.02 +/- 0.07 +/- 0.09, where the uncertainties are statistical and systematic, respectively.
@inproceedings{ORBi-b9ba26c3-cf2b-43aa-b6e5-fa66e779e11d,
AUTHOR = {Broadway, Christian and Kinet, Damien and Theodosiou, A. and Kalli, Kyriacos and Caucheteur, Christophe and Mégret, Patrice},
TITLE = {Polymer Optical Fibre (POF) Bragg gratings for Nuclear Waste Repositories},
LANGUAGE = {en},
YEAR = {08 April 2019},
LOCATION = {Paris, France},
ABSTRACT = {The Lambda(b) differential production cross section and the cross section
ratio anti-Lambda(b)/Lambda(b) are measured as functions of transverse momentum
pt(Lambda(b)) and rapidity abs(y(Lambda(b))) in pp collisions at sqrt(s) = 7
TeV using data collected by the CMS experiment at the LHC. The measurements are
based on Lambda(b) decays reconstructed in the exclusive final state J/Psi
Lambda, with the subsequent decays J/Psi to an opposite-sign muon pair and
Lambda to proton pion, using a data sample corresponding to an integrated
luminosity of 1.9 inverse femtobarns. The product of the cross section times
the branching ratio for Lambda(b) to J/Psi Lambda versus pt(Lambda(b)) falls
faster than that of b mesons. The measured value of the cross section times the
branching ratio for pt(Lambda(b)) > 10 GeV and abs(y(Lambda(b))) < 2.0 is 1.06
+/- 0.06 +/- 0.12 nb, and the integrated cross section ratio for
anti-Lambda(b)/Lambda(b) is 1.02 +/- 0.07 +/- 0.09, where the uncertainties are
statistical and systematic, respectively.},
NOTE = {Submitted to Physics Letters B}
}
Downloads: 0
{"_id":"Rj8NGsPk7rWYf7zGY","bibbaseid":"broadway-kinet-theodosiou-kalli-caucheteur-mgret-polymeropticalfibrepofbragggratingsfornuclearwasterepositories-08april2019","author_short":["Broadway, C.","Kinet, D.","Theodosiou, A.","Kalli, K.","Caucheteur, C.","Mégret, P."],"bibdata":{"bibtype":"inproceedings","type":"inproceedings","author":[{"propositions":[],"lastnames":["Broadway"],"firstnames":["Christian"],"suffixes":[]},{"propositions":[],"lastnames":["Kinet"],"firstnames":["Damien"],"suffixes":[]},{"propositions":[],"lastnames":["Theodosiou"],"firstnames":["A."],"suffixes":[]},{"propositions":[],"lastnames":["Kalli"],"firstnames":["Kyriacos"],"suffixes":[]},{"propositions":[],"lastnames":["Caucheteur"],"firstnames":["Christophe"],"suffixes":[]},{"propositions":[],"lastnames":["Mégret"],"firstnames":["Patrice"],"suffixes":[]}],"title":"Polymer Optical Fibre (POF) Bragg gratings for Nuclear Waste Repositories","language":"en","year":"08 April 2019","location":"Paris, France","abstract":"The Lambda(b) differential production cross section and the cross section ratio anti-Lambda(b)/Lambda(b) are measured as functions of transverse momentum pt(Lambda(b)) and rapidity abs(y(Lambda(b))) in pp collisions at sqrt(s) = 7 TeV using data collected by the CMS experiment at the LHC. The measurements are based on Lambda(b) decays reconstructed in the exclusive final state J/Psi Lambda, with the subsequent decays J/Psi to an opposite-sign muon pair and Lambda to proton pion, using a data sample corresponding to an integrated luminosity of 1.9 inverse femtobarns. The product of the cross section times the branching ratio for Lambda(b) to J/Psi Lambda versus pt(Lambda(b)) falls faster than that of b mesons. The measured value of the cross section times the branching ratio for pt(Lambda(b)) > 10 GeV and abs(y(Lambda(b))) < 2.0 is 1.06 +/- 0.06 +/- 0.12 nb, and the integrated cross section ratio for anti-Lambda(b)/Lambda(b) is 1.02 +/- 0.07 +/- 0.09, where the uncertainties are statistical and systematic, respectively.","note":"Submitted to Physics Letters B","bibtex":"@inproceedings{ORBi-b9ba26c3-cf2b-43aa-b6e5-fa66e779e11d,\n\tAUTHOR = {Broadway, Christian and Kinet, Damien and Theodosiou, A. and Kalli, Kyriacos and Caucheteur, Christophe and Mégret, Patrice},\n\tTITLE = {Polymer Optical Fibre (POF) Bragg gratings for Nuclear Waste Repositories},\n\tLANGUAGE = {en},\n\tYEAR = {08 April 2019},\n\tLOCATION = {Paris, France},\n\tABSTRACT = {The Lambda(b) differential production cross section and the cross section\n\t\tratio anti-Lambda(b)/Lambda(b) are measured as functions of transverse momentum\n\t\tpt(Lambda(b)) and rapidity abs(y(Lambda(b))) in pp collisions at sqrt(s) = 7\n\t\tTeV using data collected by the CMS experiment at the LHC. The measurements are\n\t\tbased on Lambda(b) decays reconstructed in the exclusive final state J/Psi\n\t\tLambda, with the subsequent decays J/Psi to an opposite-sign muon pair and\n\t\tLambda to proton pion, using a data sample corresponding to an integrated\n\t\tluminosity of 1.9 inverse femtobarns. The product of the cross section times\n\t\tthe branching ratio for Lambda(b) to J/Psi Lambda versus pt(Lambda(b)) falls\n\t\tfaster than that of b mesons. The measured value of the cross section times the\n\t\tbranching ratio for pt(Lambda(b)) > 10 GeV and abs(y(Lambda(b))) < 2.0 is 1.06\n\t\t+/- 0.06 +/- 0.12 nb, and the integrated cross section ratio for\n\t\tanti-Lambda(b)/Lambda(b) is 1.02 +/- 0.07 +/- 0.09, where the uncertainties are\n\t\tstatistical and systematic, respectively.},\n\tNOTE = {Submitted to Physics Letters B}\n}\n\n","author_short":["Broadway, C.","Kinet, D.","Theodosiou, A.","Kalli, K.","Caucheteur, C.","Mégret, P."],"key":"ORBi-b9ba26c3-cf2b-43aa-b6e5-fa66e779e11d","id":"ORBi-b9ba26c3-cf2b-43aa-b6e5-fa66e779e11d","bibbaseid":"broadway-kinet-theodosiou-kalli-caucheteur-mgret-polymeropticalfibrepofbragggratingsfornuclearwasterepositories-08april2019","role":"author","urls":{},"metadata":{"authorlinks":{}}},"bibtype":"inproceedings","biburl":"https://bibbase.org/network/files/nsSePzJcN3B2CRKPx","dataSources":["S6jBAYHh26RcqMyEJ","c7WfsT8h7KCvmbH5j","gFpEK52w5ofvoeTL7"],"keywords":[],"search_terms":["polymer","optical","fibre","pof","bragg","gratings","nuclear","waste","repositories","broadway","kinet","theodosiou","kalli","caucheteur","mégret"],"title":"Polymer Optical Fibre (POF) Bragg gratings for Nuclear Waste Repositories","year":8}