Natural Science Forum / Physics / Particle Physics / December 2006

I am puzzled as to why you think it is a "problem"?  It just seems to be
that that is the way nature is.  In a picture with the quantum "vacuum"
as a relativistic medium of virtual fermionic pairs, gauge bosons would
have to instantaneously be composed of those pairs which are bosons.  In
that case, it is better to think of gauge bosons as "wavicles" rather
than "particles".  But they would still have a particulate nature to
them due to the "medium".  Keep in mind that this is not a mainstream
viewpoint currently.

FrediFizzx

Quantum Vacuum Charge papers;
http://www.vacuum-physics.com/QVC/quantum_vacuum_charge.pdf
or postscript
http://www.vacuum-physics.com/QVC/quantum_vacuum_charge.ps
http://www.arxiv.org/abs/physics/0601110
http://www.vacuum-physics.com

Matter takes up its own room.  ?n?rjy takes up the room in between.
Thus, the latter lies in a open set.

---------------
the photon does not mediate all particles
ie if you think that it is responsible for any attraction force

2
if you find gluons (experimentally!!)   and can define their properties
**only**   by those experimental findings
please let me know ......

ATB
Y.Porat
--------------------------------

arxiver@gmail.com Wrote:

Two reasons (could be others too):
1.  If an interaction arises from Local Gauge Invariance, the particl
must transform like
\partial_\mu and therefor be a vector particle (spin one) and a boso
by spin-stat theorem.

2.  The usual basic interaction is particle-->particle + mediator.  Fo
spin addition, the mediator must have integral lspin

--
Meir Achuz

arxiver@gmail.com schrieb:

Yes, I guess that the source of this is statistics. Bosons obey to the
Einstein-Bose statistics which allows them to highly populate one and
the same quantum state. This way, bosonic interactions may combine to
result in the creation of forces which are macroscopically detectable.

OTHO, spin 1/2 particles - fermions - obey to Dirac-statistics and have
to respect Pauli's exclusion principle, which forbids 2 identical
fermions to populate the same state.

Hawkwind