possible further extensions in the new leps beamline in spring-8 s. daté accelerator division,...
TRANSCRIPT
S P r i n g8
Possible further extensions in thenew LEPS beamline in Spring-8
S. Daté Accelerator Division, SPring-8/JASRI
S P r i n g8
LEPS Collab. MeetingAcademia Sinica, Jan. 13, 2006
S P r i n g8Contents
1. Introduction2. A short summary of previous discussions on energy u
pgrade above 5 GeV 3. A new estimate of high energy gamma yield for X-ray r
e-injection scheme4. Conclusion
S P r i n g8§1. Introduction
LEPS experiments have proved the accessibility to new frontiersin hadron physics by making use of its advantages in measuring the forward angular regions without harmful background noise and manipulating gamma ray characteristics through easy-to-access laser system. They also enjoy highly stable operation of Spring-8 accelerators and its low emittance electron beams. After 5 years of physics runs with several important outputs, we are in a position to discuss a new LEPS beamline with enhancement and emphasis of recognized advantages, supplements to weak points, and challenges to completely new possibilities, which all motivated by physics.
S P r i n g8Directions of extentions
Energy -> 3.5 GeV in near future (Laser upgrade) ~> 4 - 6 GeV ?Intensity -> 107-8/s (high power laser, LRNB, high current, round beam, new tagging system)Detector Polarized target
S P r i n g8HLEP generation by X-ray re-injection (2)
8 GeV 100 mA SR
Undulator
X-ray mirrorReflectivity = 0.810 = 10%
Ex =100 eV
E< 7.4 GeV
Diamond mirror
S P r i n g8A short summary of previous discussions
X-ray generation reflection & re-injection gamma ray production
Gamma yield =
€
˙ N γ = 2Ie
e
σl
csR ˙ N ph = 4.16 ×10−12 Ie[A]
l[m]
s [mm2]Rσ [b] ˙ N ph
€
d ˙ N ph
dωdΩ= αγ 2N 2 I
e
1
ωFk (K, γθ, φ;ω /ω1)
k=1
∞
∑
€
α I
e= 4.55 ×1016 (s−1) I[A]
€
˙ N ph ≈4 ×1017 /s (100mA, N = 30)
€
˙ N γ ≈ 2 ×104 /s×l[m]
s[mm2]R
S P r i n g8
Cross section depends on photon energy
€
˙ N γ = 2Ie
e
l
csx
R ˙ I = 4.16 ×10−12 Ie[A]l[m]
sx[mm2]
R ˙ I
1 barn
€
d ˙ I
dEγ
= dωdσ
dEγ
(ω)ω1
ω2∫d ˙ N ph
dω
d˙ I dE/ I
e ,
S P r i n g8Re-focussing
Thin undulator approximation
e-
275x2 m
6x2 m
~100 rad
Can s be
€
5×10−3mm2 ?
In principle, yes.
spherical mirror
S P r i n g8Bunch mode dominance
. . .100 rad
60 cm
h ~ 275 m
e-
v ~ 6 m
€
60cm/2 ×100μrad = 30μm
€
Nγnext ~
σ
aph
~Nγ
main
5
€
Nγall ~ 1.75Nγ
main
S P r i n g8
Bunch-bunch collisions
€
˙ N γ =ne / b( )
2
sfbRI 1
€
I 1 = ˙ I Ie
e
=10−2 b (K = 5 ~ 6, Eγ = 4 - 6 GeV)
€
s = 0.5 ×10−2 mm2
€
ne / b fb =Ie
e
Limit: Heat load at finger contact ~
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ne / b( )2
fb
Maximum: 174 bunch filling
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˙ N γ = 2 ×106 /s × R
S P r i n g8Conclusion
Providedan undulator with high reflectable (R > 0.1)spherical mirror for 100 eV photonswith timing adjustment system (mirror position z = 24 +- 2 m, dz = 6mm)
€
N p = 4, λ 0 =1.1m, B0 = 300 kG − 600kG
We may obtain
€
˙ N γ = 2 ×105 /s
in principle.
S P r i n g8*******Suppl******
(2)
€
˙ N γ = ne / b( )2 fb
sx
I 1
€
=Ie
eI 1
€
˙ N γ = 2I
e
σ l
csx
˙ N ph = 4.5 ×10−14 l[m]
sx[mm2]˙ N ph
S P r i n g8Radiation formula
€
d ˙ N ph
dωdΩ= αγ 2N 2 I
e
1
ωFk (K, γθ, φ;ω /ω1)
k=1
∞
∑
€
α I
e= 4.55 ×1016 (s−1) I[A]
S P r i n g8Conclusion in the meeting on Oct. 20, 2005
The maximum yield of gamma in 5~6 GeV region attainable
in Spring-8 SR:
€
2 ×104 /s×l[m]
s[mm2]
in an 1A, 1.5 GeV SR:
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3 ×105 /s×l[m]
s[mm2]
€
K = 3, λ 0 =1.1 m
€
K = 2.56, λ 0 = 5 cm
=>
=>
S P r i n g8Cross section convoluted with Nph
†
d˙ I dE
/ R/ I
e ,
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d ˙ I
dEγ
= R dωdσ
dEγ
(ω)ω1
ω2∫d ˙ N ph
dω
S P r i n g8An undulator to produce 100 eV photons
Matching of the first harmonics:
€
K = 0.934 × B0[T]λ 0[cm]
€
100 eV = ω1(0) =4πβhcγ 2 /λ 0
1+ K 2 /2
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λ0 <1 m
€
⇒
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K = 3
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λ0 =1.1 m
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B0 = 300 kG
K > 2
S P r i n g8 Physics @workshop
Exotics: +, (1405), S11(1535) ---- 5q X(K-bound), C(1480) ---- 4q glueball, hybrid, odderon(odd-glueball) --- multi-g(+qq) Dirac monopole High precision: hyperon photoproduction nucleon resonance (e.g. pol +p 0 + p_pol ) A-dependence – mean free path nonmesonic decay of hypernucleus Compton scattering – nucleon swelling 0, –lifetime, polarizability, Primakoff (high E, forward) Others: J/ from d or A (c.f. Eth(+p J/ +p)=8.1 GeV) CP violation ()GDH polarized HD target