alejandro.rivero
May3-04, 04:52 AM
<jabberwocky><div class="vbmenu_control"><a href="jabberwocky:;" onClick="newWindow=window.open('','usenetCode','toolbar=no, location=no,scrollbars=yes,resizable=yes,status=no ,width=650,height=400'); newWindow.document.write('<HTML><HEAD><TITLE>Usenet ASCII</TITLE></HEAD><BODY topmargin=0 leftmargin=0 BGCOLOR=#F1F1F1><table border=0 width=625><td bgcolor=midnightblue><font color=#F1F1F1>This Usenet message\'s original ASCII form: </font></td></tr><tr><td width=449><br><br><font face=courier><UL><PRE>\nI am thinking a new argument for my problem. I rely in three separate\nsteps and I would like to ask opinion about each one separately:\n\n1) The self energy of a particle of mass M due to a particle of\nmass N should depend on the quotient N/M\n\nA naive argument for this is to relate compton wavelengths of both\nparticles.\nAnother possibility could be some need to truncate the summation of\nself energy contributions.\n\n2) The recoil correction for a particle of mass M bound strongly with\na nuclear conglomerate of total mass M\' should depend on the quotient\nM/M\'\n\nThis could be because the particle is not scattering from the\nnucleus, but bound around him; so the *small* momenta provided to the\nnucleus in each "quantum impulse" would redistribute itself across all\nthe nucleus. The particles in M\' are "chained" between them via the\nsame force that M, ie pions and all that.\n\n3) the combination of dependences M/M\' and N/M could as a byproduct\nhave a peak or another kind of transition when N/M\'=1\n\nWhat do you think? I wonder if there is some clue on this kind of\neffects perhaps from solid state physics or some other branch beyond\nHEP-QFT.\n</UL></PRE></font></td></tr></table></BODY><HTML>');"> <IMG SRC=/images/buttons/ip.gif BORDER=0 ALIGN=CENTER ALT="View this Usenet post in original ASCII form"> View this Usenet post in original ASCII form </a></div><P></jabberwocky>I am thinking a new argument for my problem. I rely in three separate
steps and I would like to ask opinion about each one separately:
1) The self energy of a particle of mass M due to a particle of
mass N should depend on the quotient N/M
A naive argument for this is to relate compton wavelengths of both
particles.
Another possibility could be some need to truncate the summation of
self energy contributions.
2) The recoil correction for a particle of mass M bound strongly with
a nuclear conglomerate of total mass M' should depend on the quotient
M/M'
This could be because the particle is not scattering from the
nucleus, but bound around him; so the *small* momenta provided to the
nucleus in each "quantum impulse" would redistribute itself across all
the nucleus. The particles in M' are "chained" between them via the
same force that M, ie pions and all that.
3) the combination of dependences M/M' and N/M could as a byproduct
have a peak or another kind of transition when N/M'=1
What do you think? I wonder if there is some clue on this kind of
effects perhaps from solid state physics or some other branch beyond
HEP-QFT.
steps and I would like to ask opinion about each one separately:
1) The self energy of a particle of mass M due to a particle of
mass N should depend on the quotient N/M
A naive argument for this is to relate compton wavelengths of both
particles.
Another possibility could be some need to truncate the summation of
self energy contributions.
2) The recoil correction for a particle of mass M bound strongly with
a nuclear conglomerate of total mass M' should depend on the quotient
M/M'
This could be because the particle is not scattering from the
nucleus, but bound around him; so the *small* momenta provided to the
nucleus in each "quantum impulse" would redistribute itself across all
the nucleus. The particles in M' are "chained" between them via the
same force that M, ie pions and all that.
3) the combination of dependences M/M' and N/M could as a byproduct
have a peak or another kind of transition when N/M'=1
What do you think? I wonder if there is some clue on this kind of
effects perhaps from solid state physics or some other branch beyond
HEP-QFT.