Transplanckian bremsstrahlung and black hole production
Classical gravitational bremsstrahlung in particle collisions at transplanckian energies is studied in M4×Td. The radiation efficiency ϵ≡Erad/Einitial is computed in terms of the Schwarzschild radius rS(s), the impact parameter b and the Lorentz boost factor γcm and found to be ϵ=Cd(rS/b)3d+3γcm2d+1...
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Veröffentlicht in: | Physics letters. B 2010-01, Vol.683 (4-5), p.331-334 |
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creator | Gal'tsov, Dmitry V. Kofinas, Georgios Spirin, Pavel Tomaras, Theodore N. |
description | Classical gravitational bremsstrahlung in particle collisions at transplanckian energies is studied in M4×Td. The radiation efficiency ϵ≡Erad/Einitial is computed in terms of the Schwarzschild radius rS(s), the impact parameter b and the Lorentz boost factor γcm and found to be ϵ=Cd(rS/b)3d+3γcm2d+1, larger than previous estimates by several powers of γcm≫1. This means that in the ultrarelativistic case radiation loss becomes significant already for b≫rS, so radiation damping must be taken into account in estimates of black hole production at transplanckian energies. The result is reliable for impact parameters in the overlap of γνrS |
doi_str_mv | 10.1016/j.physletb.2009.12.042 |
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The radiation efficiency ϵ≡Erad/Einitial is computed in terms of the Schwarzschild radius rS(s), the impact parameter b and the Lorentz boost factor γcm and found to be ϵ=Cd(rS/b)3d+3γcm2d+1, larger than previous estimates by several powers of γcm≫1. This means that in the ultrarelativistic case radiation loss becomes significant already for b≫rS, so radiation damping must be taken into account in estimates of black hole production at transplanckian energies. The result is reliable for impact parameters in the overlap of γνrS<b<bc, ν=1/2(d+1), and b>λC, with bc marking (for d≠0) the loss of the notion of classical trajectories and λC≡ℏ/mc being the Compton length of the scattered particles.</description><identifier>ISSN: 0370-2693</identifier><identifier>EISSN: 1873-2445</identifier><identifier>DOI: 10.1016/j.physletb.2009.12.042</identifier><language>eng</language><publisher>Elsevier B.V</publisher><subject>General Relativity and Quantum Cosmology ; High Energy Physics - Experiment ; High Energy Physics - Phenomenology ; High Energy Physics - Theory ; Physics</subject><ispartof>Physics letters. 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The result is reliable for impact parameters in the overlap of γνrS<b<bc, ν=1/2(d+1), and b>λC, with bc marking (for d≠0) the loss of the notion of classical trajectories and λC≡ℏ/mc being the Compton length of the scattered particles.</description><subject>General Relativity and Quantum Cosmology</subject><subject>High Energy Physics - Experiment</subject><subject>High Energy Physics - Phenomenology</subject><subject>High Energy Physics - Theory</subject><subject>Physics</subject><issn>0370-2693</issn><issn>1873-2445</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2010</creationdate><recordtype>article</recordtype><recordid>eNqFkE1Lw0AURQdRsH78BcnWReKbN8kk2VmKWqHgpq6H6cwbM22ahJm00H9vS9WtqweXey68w9gDh4wDl0_rbGgOsaVxlSFAnXHMIMcLNuFVKVLM8-KSTUCUkKKsxTW7iXENALwAOWHlMuguDq3uzMbrLlkF2sY4Bt20u-4r0Z1NVq02m6TpW0qG0NudGX3f3bErp9tI9z_3ln2-vixn83Tx8fY-my5SI3I5phoduhIcVJycIKysESAQEMkIy_OixAJJOlE7NKWopXS5EZXVBRdkjRG37PG82-hWDcFvdTioXns1ny7UKQOQHHld7fmxK89dE_oYA7k_gIM6qVJr9atKnVQpjuqo6gg-n0E6frL3FFQ0njpD1gcyo7K9_2_iG2XsdZw</recordid><startdate>20100125</startdate><enddate>20100125</enddate><creator>Gal'tsov, Dmitry V.</creator><creator>Kofinas, Georgios</creator><creator>Spirin, Pavel</creator><creator>Tomaras, Theodore N.</creator><general>Elsevier B.V</general><general>Elsevier</general><scope>AAYXX</scope><scope>CITATION</scope><scope>1XC</scope></search><sort><creationdate>20100125</creationdate><title>Transplanckian bremsstrahlung and black hole production</title><author>Gal'tsov, Dmitry V. ; Kofinas, Georgios ; Spirin, Pavel ; Tomaras, Theodore N.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c346t-a2f2f70f081ef3e28dc3032022ec3d1457252e6f39f2c73966f4c38da513edcc3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2010</creationdate><topic>General Relativity and Quantum Cosmology</topic><topic>High Energy Physics - Experiment</topic><topic>High Energy Physics - Phenomenology</topic><topic>High Energy Physics - Theory</topic><topic>Physics</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Gal'tsov, Dmitry V.</creatorcontrib><creatorcontrib>Kofinas, Georgios</creatorcontrib><creatorcontrib>Spirin, Pavel</creatorcontrib><creatorcontrib>Tomaras, Theodore N.</creatorcontrib><collection>CrossRef</collection><collection>Hyper Article en Ligne (HAL)</collection><jtitle>Physics letters. B</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Gal'tsov, Dmitry V.</au><au>Kofinas, Georgios</au><au>Spirin, Pavel</au><au>Tomaras, Theodore N.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Transplanckian bremsstrahlung and black hole production</atitle><jtitle>Physics letters. B</jtitle><date>2010-01-25</date><risdate>2010</risdate><volume>683</volume><issue>4-5</issue><spage>331</spage><epage>334</epage><pages>331-334</pages><issn>0370-2693</issn><eissn>1873-2445</eissn><abstract>Classical gravitational bremsstrahlung in particle collisions at transplanckian energies is studied in M4×Td. The radiation efficiency ϵ≡Erad/Einitial is computed in terms of the Schwarzschild radius rS(s), the impact parameter b and the Lorentz boost factor γcm and found to be ϵ=Cd(rS/b)3d+3γcm2d+1, larger than previous estimates by several powers of γcm≫1. This means that in the ultrarelativistic case radiation loss becomes significant already for b≫rS, so radiation damping must be taken into account in estimates of black hole production at transplanckian energies. The result is reliable for impact parameters in the overlap of γνrS<b<bc, ν=1/2(d+1), and b>λC, with bc marking (for d≠0) the loss of the notion of classical trajectories and λC≡ℏ/mc being the Compton length of the scattered particles.</abstract><pub>Elsevier B.V</pub><doi>10.1016/j.physletb.2009.12.042</doi><tpages>4</tpages></addata></record> |
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subjects | General Relativity and Quantum Cosmology High Energy Physics - Experiment High Energy Physics - Phenomenology High Energy Physics - Theory Physics |
title | Transplanckian bremsstrahlung and black hole production |
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