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Astrophysical
QuarkMatterRenxin
Xu(徐仁新)School
of
Physics,
Peking
University2005年10月12日,扬州大学“Astrophysical
QM”/rxxu➢imagine,
it
is
stranger
than
we
can
imagin➢——
ArthurEddingtonAstrophysical
laboratory:
to
find
QGP?·Cosmic
QCD
phase
separation:
consequence?·Compact
pulsar-like
stars:
quark
stars?·Cosmic
rays:
quark
nuggets?“Astrophysical
QM”/rxxuSUMMARYIntroduction:
quark
&
quark
matteQM
in
the
earlyUniverseQM
in
pulsar-like
compact
starsQM
as
cosmic
raysConclusions“Astrophysical
QM”/rxxuQuark?
A
historical
note
…M.
Gell-Mann
(1969)Quarks?1950s~1960s:
A
success
inthe
classification
of
hadrondiscovered
in
cosmic
rays
andin
acceleratorsM.
Gell-Mann
(1964):Quarks?
----
in
mathematicaldescription,
rather
than
inreality.Zweig,
Chinese
group(1960s):
in
reality?1973:
SU(3)
non-Abelianasymptoticgauge
theoryfreedomExperimental
evidence
forthe
last
flavor
of
quark
(topquark)
in
1990sIntroduction:
Quark
matteruThe
standard
model
ofparticle
physicsInteraction
via
gauge
bosQCD“Astrophysical
QM”/rxxuuExperimental
evidence
for
asymptotic
freedIntroduction:
Quark
matter“Astrophysical
QM”/rxxuM.
R.
Pennington
(University
of
Durham)
in:
QCD
aHadronic
Physics
(Held
in
PKU,
Beijing,
June
20,The
Nobel
prize
in
Physics
(2004)David
J.
Gross
(L)
of
theUniversityof
Californiaat
Santa
Barbara
and
hiswife
(R)Frank
Wilczekof
theMassachusettsInstitute
ofTechnology.H.
DavidPolitzer
of
theCaliforniaInstitute
ofTechnology,Pasadena,California.uWhat
is
Quark
Matter?ÞExpectedin
QCDIntroduction:
Quark
matter(Hadron
gas)To
be
a
direct
consequence
ofaympt.
freedomA
simple
QCD
phase
diagram(QGP)“Astrophysical
QM”/rxxuCan
we
find
quark
matter?·Terrestrial
experimentsÞRelativistic
heavy
ion
collide·Astrophysical
observationsÞT-dominated
QM:
earlyUniverseÞD-dominated
QM:
compact
starsIntroduction:
Quark
matter“Astrophysical
QM”/rxxuuSolid
Quark
Matter?Introduction:
Quark
matterBSolid?Liquid?Gas?HadronQGP0QCD
phase?TPhase
diagram
for
CO2“Astrophysical
QM”/rxxuuTwo
kinds
of
Quark
Matter.Solid
QM?T-dom.D-dom.Introduction:
Quark
matterXu
2005“APAPsusutltlrsrsoaoarprphshsyasnidcQaulaQrMk”Starhst”tp:h/t/tvpe:g/a/.vbeagac.pbkauc.epdku.cend/ur.xcxnu/rxSUMMARYIntroduction:
quark
&
quark
matte√
QM
in
the
early
UniverseQM
in
pulsar-like
compact
starsQM
as
cosmic
raysConclusions“Astrophysical
QM”/rxxuEdward
Witten
(1984):1,
cosmic
QCD
phase;
2,
strange
stars;
3,
cosmicrayQM
in
the
early
Universe“Astrophysical
QM”/rxxuuBodmer-Witten’sconjectureeumu
~
5umd
~
10ums
~150u
=1.5Nu
F
~
400uFarhi
&u
Jaffeu
(1984)Greiner
et
al
1998Introduction:
Quark
matter“Astrophysical
QM”/rxxuCome
back
whenwe
discuss
p-pdot
diagramB
critical
=
4.4x10^13
GQM
in
the
early
UniverseSchwarzastro-ph/0303574Quark-hadron
phasetransitiont
~
10-5
s,
Tc
~
300
MeVFirstorderS.
Banerjee,
et
al.hep-ph/0307366reheating“Astrophysical
QM”/rxxuCome
back
whenwe
discuss
p-pdot
diagramB
critical
=
4.4x10^13
GQM
in
the
early
UniverseMotivations
to
study
quark-hadron
transit“Astrophysical
QM”/rxxuto
know
“What
happened
at
thetransition?”to
set
initial
physical
conditions
for
Binhomogeneous
distribution
abundanceto
generate
relics
of
cosmic
QCD
transitstrange
quark
nuggets?
(MACHOs?)gravitational
waves
from
colliding
bubbmagnetic
fields
with
~
100
kpc
correlatiQCD
balls
as
a
new
CDM
candidate?black
holes
formation
during
the
transitSUMMARYIntroduction:
quark
&
quark
matteQM
in
the
earlyUniverse√
QM
in
pulsar-like
compact
starsQM
as
cosmic
raysConclusions“Astrophysical
QM”/rxxuA
historical
note
of
pulsarsDegeneratepressure
is
notomnipotent
instanding
against
thegravitationalcollapseMaybe
thereare
stars
withnucleardensity
aftercollapse?“Neutron”starS.
Chandrasekhar
(1983)L.
Landau
(1962)“Astrophysical
QM”/rxxuWalter
Baade
and
Fritz
Zwickyproposed
in
1934
that
supernovaecould
produce
cosmic
rays
andneutron
stars
…A
historical
note
of
pulsarsPulsars(discoveredin
1967)could
beneutronstars?A.
Hewish
(1974)“Astrophysical
QM”/rxxuPulsars
in
conventional
scenariouRadio
pulsars:
cosmological
lighthousePulse
sequences
from
a
radio
pulsarPulsar
is
pulsing
…“Astrophysical
QM”/rxxuCome
back
whenwe
discuss
p-pdot
diagramB
critical
=
4.4x10^13
GsNeutron
StarorQuark
stars?Pulsars
in
conventional
scenario“Astrophysical
QM”/rxxuPulsars
in
conventional
scenariouDistribution
of
radio
pulsars
in
the
Gal“Astrophysical
QM”/rxxuRadio
pulsarsAccretion-powered
X-raypulsarsX-ray
burstsAXP/SGRDim
thermal
“Neutron”
starsCompact
centerobjectsMembers
of
the
family
of
pulsar-like
stars
…What’s
reallythe
nature
ofpulsars?“Astrophysical
QM”/rxxuHeiselberg
2002uThe
structure
of
normal
Neutron
starsAtmosphereOuter
crustInner
crustNeutron
matterCore?QM
in
pulsar-like
compact
stars“Astrophysical
QM”/rxxuuPul➢sIavrasne:nqkuoa&rHkusrsdtgaerlsa?idze
(1969)Itoh
(1970)Bodmer
(1971)Asymptotic
freedomWitten
(1984)1986:
Haensel
et
al.;
Alcock
etal.QM
in
pulsar-like
compact
stars“Astrophysical
QM”/rxxu/photo/2002/0211/0211_illustration.uNeutronStarsuv.s.uQuarkStarsQM
in
pulsar-like
compact
stars“Astrophysical
QM”/rxxuCome
back
whenwe
discuss
p-pdot
diagramB
critical
=
4.4x10^13
GuTwo
requirements
for
forming
quark
starQuark
de-confinement
can
occurAnestimateof
c:(4 R3/3)-1
~
1.5NStrange
matter
in
bulk
is
absolutely
sta (Bodmer-Witten’s
conjecture)Note:
Strangelet
in
RHIC
could
be
unstable!uUnfortunately,
one
can
not
know
if
thesetwo
are
satisfied
from
the
first
princip(QCD).
But
the
requirements
seem
ok
…QM
in
pulsar-like
compact
stars“Astrophysical
QM”/rxxuuStructure
of
strange
star:
bare
or
crusElectric
field:E
~
1017V/cmQM
in
pulsar-like
compact
stars“Astrophysical
QM”/rxxuHow
to
form
a
quark
star?QM
in
pulsar-like
compact
stars“Astrophysical
QM”/rxxuIt
is
still
a
challenge
for
astrophysicistsreproduce
asuccessful
core-collapse
superWhat
if
to
form
a
quark
star,
rather
tha
a
neutron
stars,
in
a
CC-process?This
idea
is
attractive
since
more
ener
and
radiation
(
,
)
are
released
…Note:
quark
stars
formed
in
this
way
should
be
baQM
in
pulsar-like
compact
stars“Astrophysical
QM”/rxxuCome
back
whenwe
discuss
p-pdot
diagramB
critical
=
4.4x10^13
GQM
in
pulsar-like
compact
starsEvidence
for
quark
stars?A
summary
of
our
work
only
…“Astrophysical
QM”/rxxu·To
solve
the
binding
energy
problem
(199ÞObservations:
drifting
subpulses
of
P·To
expect
non-atomic
spectra
(2002)ÞObservations:
thermal
&
non-thermal·To
explain
discrepancy
between
…
(2004ÞObservations:
free
prec.
&
glitch
of
P·To
understand
others
…ÞObservations:
superE
SGR,-profile(AG)QM
in
pulsar-like
compact
stars“Astrophysical
QM”/rxxuCome
back
whenwe
discuss
p-pdot
diagramB
critical
=
4.4x10^13
GNASA
News
release
(2002/4/10):
RX
J1856
a
strange
stChandraQM
in
pulsar-like
compact
stars“Astrophysical
QM”/rxxuCome
back
whenwe
discuss
p-pdot
diagramB
critical
=
4.4x10^13
GHow
to
identify
clearly
aquark
st·Submillisecond
radio
pulsar:
FAST?·Low-mass
&
small-radius
pulsar-like
stars:
X-ray
interference
telescopes
MAXIM?·Gravitational
wave
observations:
LIGO·Dust
emission
from
ms-pulsars:
SpitzeQM
in
pulsar-like
compact
stars“Astrophysical
QM”/rxxuI
amintroducing
youFive
hundred
meter
Aperture
Spherical
TelescQM
in
pulsar-like
compact
starsI
amintroducing
you“Astrophysical
QM”/rxxuSUMMARYIntroduction:
quark
&
quark
matteQM
in
the
earlyUniverseQM
in
pulsar-like
compact
stars√
QM
as
cosmic
raysConclusions“Astrophysical
QM”/rxxuQM
as
cosmic
raysThe
higher
the
particle
energy
attained,
thethe
scale
of
physics
which
can
be
probed.Cosmic
rays
vs.
Particle
physics√1937
(Anderson
&
Neddermeyer):√1947
(Powell):√1947(Rochester
&
Butler):
strange
part.0,
K,
...Cosmic
rays
vs.
Astrophysics√Generally,
astrophysics
studies
“cosmic√Astrophysics
offers
extreme
environments“Astrophysical
QM”/rxxuUHECRs:>~1019eVuThe
highesWithin
theGalaxyQM
as
cosmic
rays“Astrophysical
QM”/rxxuuGZK
cutoff:
estimationsuEp
~
Ep/1GeV
~~
1019
eV,1010uECB
~
3
K
~
10-4
eVProton
rest
frameE’CB
~ ECB
~
MeVGreisen
PRL
(1966);
Zatsepin
&
Kuzmin
JETP
(19QM
as
cosmic
rays“Astrophysical
QM”/rxxuCome
back
whenwe
discuss
p-pdot
diagramB
critical
=
4.4x10^13
GuThe
GZK
cutoffwith
thresholduOther
particlesPhoton,IronQM
as
cosmic
rays“Astrophysical
QM”/rxxuStecker2003QM
as
cosmic
raysuNo
clear
GZK
cutoff
observed“Astrophysical
QM”/rxxuCome
back
whenwe
discuss
p-pdot
diagramB
critical
=
4.4x10^13
GuUHECRs:
quark
nuggets
(strangelets)?uWhat
is
Strangelet?=>A
lump
of
strange
mattuAdvantages
if
UHECRs
are
strangelets:Larger
mass Beyond
GZK
cutoffML03Higher
electricityBe
not
point-likeEasier
to
accelNo
collapse
to
B(Xu
&
Wu
2003)“Astrophysical
QM”/rxxuQM
as
cosmic
raysCome
back
whenwe
discuss
p-pdot
diagramB
critical
=
4.4x10^13
GuWhat
is
the
astrophysical
origin
of
stranduring
the
early
Universe?during
the
formation
of
quark
stars!√Acceleration
in
induced
electric
field
~
1017/P1√Formation
by
stellar
processes1,
Evaporation
during
SNEs2,
Collision
of
(low-mass)
strange
QSGRBsQM
as
cosmic
rays“Astrophysical
QM”/rxxuCome
back
whenwe
discuss
p-pdot
diagramB
critical
=
4.4x10^13
GuHow
do
strangelets
evolve
in
the
atmospheSolid
strangeletFluid
strangeletEvaporatinghadrons:
n,
p,
..QM
as
cosmic
rays“Astrophysical
QM”/rxxuCome
back
whenwe
discuss
p-pdot
diagramB
critical
=
4.4x10^13
GuHow
can
we
detect
strangelets?Atmospheric
Cerenkov
radiation?Atmospheric
fluorescence
radiation?ESA:
in
YBJ?Neutron
detection
in
YBJ?…?QM
as
cosmic
rays“Astrophysical
QM”/rxxuCosmic
raydetectionin
YBJSUMMARYIntroduction:
quark
&
quark
matteQM
in
the
earlyUniverseQM
in
pulsar-like
compact
starsQM
as
cosmic
rays√
Conclusions“Astrophysical
QM”/rxxuConclusions·Astrophysical
quark
matter
are
reviewed.
Inadditio
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