synchrotron light source data book
TRANSCRIPT
BNL--42333
DE89 014499
SYNCHROTRON LIGHT SOURCEDATA BOOK
j lm murphybnl/nsls
MIM Of IHIS nor.HWEHT IS UNLIMITED
DisclaimerTins repon was prepared as an account of work sponsored by anagency of live United Stales Government. Neither the UnitedSuites Government nor any agency ttwreof, nor any of theiremployees, nor any of their contractors, subcontractors, or theiremployees makes any warranty, express or implied, or assumesany legal liability or responsibility for the accuracy, complete-ness, or usefulness of any information, apparatus, product, orprocess disclosed, or represents that its use would not infringeprivately owned rights. Reference herein lo any specific com-mercial product, process, or service by trade name, trademark,manufacturer, or otherwise, does not necessarily constitute orimply us endorsement, recommendation, or favoring by theUnited Slates Government or any agency, contractor or subcon-tractor thereof. The views and opinions of authors expressedherein do not necessarily state or reflect those of the UnitedState* Government or any agency, contractor or subcontractorthereof.
i/ivFOREWORD
The "Synchrotron Light Source Daw Book" is as iu nameimplies a cnlleciion of dam on existing and planned synchrotronlight sources. 1 1 K intention was to provide a compendium oftools for the design of electron storage rings as synchrotron radi-ation sources. The slant is toward the accelerator physicist asother booklets such as iltc X-Rny Data Booklet, edited by 1)Vaughan (l.BL PUB-490), address I IK 'use' of synchrotron radi-ation. 1> is hoped that the booklet serves as a pocket siwd refer-encc to facilitate back of the envelope type calculations. It con-tains some useful formulae in 'practical units' and a brierdescription of many of the existing and planned light source lat-tices.
1 welcome corrections and suggestions for improvement. If aparticular machine is missing it is because I did not have readyaccess to the data. Additional machines will be added as litedata becomes available.
I would like to thank my colleagues for providing the datafor the various lattices. In particular 1 would like to thank Dr.Vukihide Kamiya (KEK) for gathering the information on mostof the Japanese machines. The computer code LEDA authoredby Dr. Gactano Vignola (BNL) was used to generate the latticedisplays.
James B. MurphyNSLS 725CUpton, New York 11973January [email protected]
Table of Contents
1 rorcword in
2 Nomenclature & Physical Constants I
3 Useful Formulae .
4 Orthogonal Curvilinear Coordinates l
5 Synchrotron Kwiiation Integrals I
d Closed Otnii Errors <
7 Random FJTOTS (>
H Storage Ring linullaih'r "I
** Beam Size and Angular DivvrgeniT H
10 fcteciron Hcflm Optics A Twiss Parameters y
11 Maynclic Mult iples 10
12 Radio Frequency System II
l!> Chmmaticiiy 12
14 Hctatron Resonances 12
15 FJectron fleam Liteiimc 14
16 Synchrotron Radiation 15
17 Utulubtors IX
IK Wipglers 21
19 Umlula lor Field Versus G a p 22
20 Effects of Planar Insertions on the Ring 23
21 Synchrotron Ltj;ht Sources Worldwide 24
22 Storage Ring Lattices 27
2.1 Addresses K8
24 References VII
( I
'1V,
r,X,ca,J,II
r,Xa,,nh
Nomenclature
momentum cmnpacltondispersion functionbetatron tunecritical ertcrpydamping timecircumtt'a'rK.venergy .spa'ik)pailitiou fuiKiionsriturant-Snyik'r lnv;uianiTotal Cowercniiilancc couplingnn\ beam si/clicltl niik'ik
RF lurmoniL* numberundulator period
P,a,.|i,.Y,\Pli1:F
f , ,•
Vi
tS,
°A •'
/v,K
txM.llro.l l l l lKl l
Twis\ par.tnu't'cniical waM'K1
di]M)k' fviutmt!ruac'K'IK. tic-lilenergyemillaiui'initiation li^v'i'
cliroin.'tlK'iuRF aiveplaiuoangular spteadquadru|i»lr M Kphntun ftuxiindiilaliu parai
r . i . i i u v
MCII Quaniny Svnibnl
IZIemcntary ChargeElectron MassProton Mass
Planck ConstantSpeed of LightClassical Electron RadiusFine Structure ConstantBollzman ConstantPermittivity of Free Space
Permeability of Free Space
Impedance of Free Space
c
'"tr
hc
'.ak
e«Hozu
1«)22xlir|li
V l(NSxK) Vl
1.6726x10 ;?
6.6262xl(rM
2.W79XI0"2.8179x10""1/137.041.3807x10-"R.8.142X1O"'1
4itxlO"7
376.73
meter
jnule/1 Kfarad/in
lienn/mnlinis
Simii' I'wful lorinuUr
'; Hl = — IK til
i n / • K,vi
1 " i ' i pi'" i
lAvi I M . S /••' i < i r r | « i ; i
'' ' 11i • • .««•
I (,-M)1' / |(,V>
^ ^ J ' " ' ' 1 • i'\m\ r , , | A . ' i - | n ^
i*:^/V"-. |
/C = >H4 /(, | ; | X, |<™l
| . m |(i + — •
| \ , A ;
ul dmil int iar Coorflinal
Aff J^nplli A Volume I'k'nu'M
i l l * = h f«/u |* + hutul *» i WH { */\ •- h th jh tftu
(irjilicnt
V.I =
Cult
d ^2^( ) •+ permui(itmn\
Coordinate System
CanesianI Cylindrical' Spliencal
F-'rc'iiM-Sfnt'l
* 111
11
11r sinO
il * X'PJ
" 1X
rr ^X
y0
t i//? ,s
Synchrotron Radiation Integrate"''
I,-- | -^d.t . / ; = J -V<A . / , = | — ~ d s
j - , , , A r 7 ^ ' " ^ . ' P 7 -
1 I NUmiciHuni coinpaciinn: n = —7
2 1 Uni'usy loss per lunv t/(l = TV'
3 t Damping panilion functions: Jt - I and Jt = 2 + —
55 * \ F. Y ')4,Ene,gy,p«»1|:oI'.^--^j1j-t7-
5.,Emi.un«:c--^-!.f-£ ^ -'»[mrJ J ' j - ' t
6 ) Damping limes: T, (msl = C t m l P l m ) ^
Closed Orbit Errors'"" '•*"•*•'
A single point kick of strength, y , at s = 0 along the cir-cumference of a storage nng gives rise to a closed orbit dis-placement at position s.
where p(0) and P<i) arc the betatron functions at the location ofthe kick and the observation point respectively, • ( T ) is the phaseadvance from the kick to Ihe observation point and v is the beta-tron tune.
The angular deviation is obtained simply by diffc;cn!tation,
^ l ' " 2 V p<5) sinicv
where O ( J ) = - P ' ( I W .
Kicks can arise from dipole trim magncls or errors in themain magnets. The table below lists some of the kicks due tomagnet errors assuming the betatron phase advance across tlicdisplaced clement is small.
I t:lcmcni TvpcQuiulrupole ofIfngth.L. &
• Strength.**2
Uipolc of An>!lc,Q
Uipolc cif Aii(;le.<>
Source of Kick
Displacementby d, ,
Rotation by 0
Reid Error. —a
VK-I.A, ,
Plane
x.y
_J.X
II tbc plia\c ailvantc alonp (IK kick is not small, i.e.vl.v'i r v S o ' l . the closed orbit must be deienmneil (rom tin-innp.' general ct^uation for an extended kick.
The closed orbil blows up for integer tunes indicating ilk'existence of a icsonancc for v = integer.
The bewron lune shift due to a gradient error 5K* is givenby
Tlw change in the hclalron function is given by
A p ( J ) = • • • f t j J - f 6 A ' 2 U ' )P( .V ' ) cos2((jK.v ) - • < * ' ) -2 s in2xv £
Die betatron functions blow up for half integer tunes indicatingthe existence of a resonance for v = intcgcr/2.
Kandon Errors: Closed Orbit Amplification Factors1'"1 <;v'
P, and P,, arc defined to be llw ratio between I ho closedorbit distortion at a particular location which will not beexceeded with 9S% probability, to the 'rms error' in alignmentof the elements.
For quadrupoles. the error is the rms displacement of the elc-meni assumed to be the same for all quads.
For dipoles of bend angle $ ; . P, is the 98% ratio betweenclosed orbit distortions in meters and the relative rms field errorsAB/B; similarly P, is the ratio between closed orbil distortionsin meters and the rms lilt of the dipolcs.
Kmillwwe IN An Kitrtron .Storage King
In an electron storage ring, with an isomapnclic guide livid,the horizontal cniiilance of the electron beam is given by"''.
whore H ~ yt\\? + 2aAn^l , ' + P t V " .
j _ Jj
I for « .wi7r*r nuinwt0 f(M" (/ pantlh'l magnet
ami
„ « _ £ . i £ , r , . - 5 2 L - = 3.WX 1 0 ' V. -ra./. (41
In general a light source lattice is constructed from 'basiccells ' . A cell contains dipolcs. quadrupnlcs and se.Mtipnlcs andis usually bounded by di.spcnion free drift spaces for inseriiondevices.
To explore the differences between the various types of lat-tices it is useful to rewrite ( I ) as
E = F(vx Janicr) * I ^ • m -rod (51
wlicre N j is the number of dipole magnets. !•* is the eiKTgy inGeV.
For a tixed Nrf & E the main variation in t5i is due to F :iv,.lattice), since 0 < Jt < 3 and is typically J, - \-2. Hie follnuing table lists the approximate minimum values of l ; <v, i tnrseveral types of lattices. A realistic lattice "ill have a slij;hil\
higher value lhan the theoretical minimum* given here. ThelaMe also mentions an example of c.ich latiice type to give thereader an idea of the basic eel! and the betatron and dispersionfunctions. Tl\e emitlances for these example rings arc not neces-sarily given by Ihe minimum value.
Lattice Tvpe
FODO"ChasmanGreenTriple Bend AchromulThcor. Mininuim Emit.
mm7.2K2XIO""1
1.36x10"*
r 7.S4XKI""
Ayccllt
T
31
ExamplePF.PNSLS VUVBESSY II
dispersion suppressors must nc added to yield n, = 0 insertions
References: Hc2. Kal. Ril, Sol , Tel . Wil
Beam Size and Angular Divergence
The horizontal and vertical bcamsizes are given by.
The horizontal and vertical angular divergences arc given by.
Lwherr 7,
1 + a , 2
- . and
X is defined lo be the cmittance coupling.
Kleclnm Htam Optic* & Twiss Parameters"''
The particle position and angular deviation arc pven t\v.
''<•'> = -\l-^— Nl lcnMVl i t • 01 + Mill VI >> • 01J
yl.i k'os|X<' i » 0i
X(A) satisfies tan l¥(.t) - %U)1 = The trio (a, | i . v) arc
rcferrx'ti in as the Twiss ponuncfL*rs.
The invariant cmituutcc ellipse w given by
,- slope=- -ii-
[-« x'int
• Iransfonn tlte ellipse u> a circle the follttwing nonnali/eilles are useful.
X = •
Magnetic Mullirwfcj*''•*'•
lor a magnetic ticltt with 'median plane symmetry", tlie heldi.HI he expressed, in lite source free region, as 8 = V<l> w litre <1>is a solution ot lite 3 dimensional Ljflacc equuium V*4> ~ 0 inv ur\ iline.ii UHUilinales.TWII Dimensional Ideal Mullipole Mumls
I oi an ulc.tl mullipole. assuniinc (he rr.ajjiicl is siraiptu<i > <•>) and itziuuint: Irin^ui^ liekis. ific mu^nctic field is puii'lyit.uiNXL'ise {I diini'MMiinal) and the stvluthin lo ilic l^ipliiLi* cquaiir-n cm tv wrmen ;is,
m i)A.sinimOll
1 m i classes ot imilnpoles ansc lUMuralty from this expansionami they are catalogiii-il in the laMe below for in = 1. 2. 1.Pure Regular Multipoles («„ = (), bm * (1)
Multitude <t>
' Dipnle f',v
Quadruptile 2ft»i.v
h,
Puie Skew Mulnrxiles lnm » {), bm = 0)
i MullipoleDipoleQuadnipoleSe\tu|>ole
B,0
- \ "I Ni ,11
J
A regular multipole is oriented such that u produces only Jvciiica) tic!J compoiK'ni iti llie median plane (y = 0) A regularnuilii[>«)lc vuiti 2ni poles is itaiiNlumieil to a skev. tiuilliptile hy anii.iiitui n| 0 = n/fin .lUnii the axis of the ma tH.-;
Errors In Mulliptile Magnets1":
If Ihe symmetry of Ihe 2m pole magnet is prcsoiuNl di yconstruction and the imperfections arc due only u> iht' uuiuaut'tiof Ihe equipolcnlial surface of lite mm lamination, tlie .illim.ihlrmultipole errors contain 2n = 2m(2k * 1) poles »uh k I.."1
For example:
I Muliinole Allowable KnotsI Dipole Scxtupolc (6 pole I. IX-capi>te (10 |H>le) ciiI Quadrupole IXxlecapole (12 pole), (20 pule), cii.| Scxiupole (IK pole). j M _ M y ; etc_
If the symmetry of Ihe mapici is broken ilk' typenumber of multipole errors can he much yn-aici aiut L'.K II <must be examined in detail.
Radio Frequency System^'
1.) Synchronous Phase, 0 i :
i " o , 1
• , = sin ' | - ^ — | - vin |—|
2.) RF Acceptance. E W :
'IF ~ ± —(*'</* - I - c o s '(!•'</ II[nahIC
i.) Synchrotron Tune, v,:
n,4.) Bunch Length, O t :
' 2n/i IU •o, =
Chn>mailclly'M'
L- M <b IP, {K2 - 2h- - 2K2hr\, - r n , - A'n, ')4n^
= -^-7 IP> <-*2 + K2hr\, +ri\, + h'r\,') +4HJJ
},] ds
Betatron R«on«ncss*' :
Resonances in die panicle's bctairnn molion occur when tin'luncs satisfy:
m v , + n v , = p N,
where m.n.p & N are integers, | m | • |n | is I IK order of theresonance and
{^i .uruclurr resoruwcf<;.
I ruin-structure resonances
Resonances are further classified as 'regular' or 'skew*depending on whether the resonance is driven hy a regular orskew multipole. Sum resonances arc of greater concern thandifference resonances. The accompanying figure is a typicaltune diagram indicating all regular multipole resonances up toorder 4 assuming N = I.
For a low cmituncc light source lattice the most importantresonances arc the third order regular sextupole driven reso-nances:
3v, = pN <t v , + 2vv = qH
Regular Resonances Up to Order 42.0
1.8
1.6
1.4
1.2
1.0
'Z
i »
c
3.0 3.2 3.4 3.6 3.8 4.0
Second --- Third Fourth
Electron Beam Lifet ime" '•"';
The gas scattering lifetime has contributions from elaMK'scattering of the stored beam on nuclei.
and due to brcnisstiahlung on nuclei,
I ttvr:Z:p<
In hJTJT <-'«r« - ™>
where p and Z arc the nuclei density and choice rcspecmcU. .1and h aie the hnnznnial »"'' vertical stay clear apertures and i K,is the radio frequency acceptance.
The Touscliek lifetime is given by,
I • / « r ; <• N ( i t )
where V = KKv 2<j,o,a,. C =
trons per bunch andI".
, N is the number of clec
2 f « 2 v «
The smaller of the physical, radio licqucncy or dynamicacceptance should be substituted for taii • Because tlie Touscheklifetime depends on (he machine funcnons 11 should he computedas a weighted average around the entire nng.
The quantum lifetime is given by.
where % = t}Ft2of.
Synchrotron Kadiitlon '
The radiation emitted by a relativistic electron in a magneticlickt is called synchrotron radiation. The radiation emitted has at>m*l spectrum fix low photon energies and falls off eiponcn-dally above the critical photon energy, Er = ftcuf = 3tu-y\2p.
e,|/CcV] = .665 8(7 1 E2{CrV\. (Is)18 64
K 1 1 = k lib)B\T)F.:\aeV)
Half of the total power is radiated above the critical plioionenergy and half below. Due to the rclativistic motion of theelectron the radiation is highly collimated in the forward direc-tion with a characteristic vertical opening angle,
(2)
Y (i)
Y 'I aK ,n
—( ) . (il » «),Y di
The spectral and angular distribution of photons is given by:
~dh~
with units of (photons/sec/sieradianl, I in amps, e = 1.6x10"" Cand where i, = oi(l + Y3V2)3/2/2<or. The first term in the squarebracket corresponds to radiation polarized in the plane of theorbit and (he second term to radiation polarized perpendicular tothe plane.
In the forward direction (y = 0) the above can be written inpraclical units as:
•jjy = I..125x10" -5H E'ICV] I \Amp]HXym (4)
with units of (photons/scc/ninMHWw»dv|. y • <aliae = \efk andH:(y.O) = y2Kfn{yl2i is plotted in * c accompanying figure.
If «jn. (.1) is integrated overall venical angles one obtainsIIH1 llun per milhradun of horizontal arc.
1 , - 9 . , J A-,,(,,Wl.
with units of Iphoiuns/sec/nirad 6], I in Amp & e = l.6x!0~ig C.
In practical units this can be written as
• ^ = 2.4S7xlOlft£ \GcV\l \Amp\C,{y) —. (6)JO o)
with units of [pruilons/scc/nirad 8| and where
<7 ,(v I = v j «Tj,,(4 tdi (7 |>
Figure 1 is a plot of t)ie functioffi Hjiy.O) and Ctt(y). Figure2 iv a plot of dN/d8 as a function of photon energy fix radiationI mm a representative range of storage rings.
T I K total power radiated is given in SI units by,
*xr.mc2
p, = '
or in practical units hy.
/ ' ,(*» I = Ua\KeV\l\Amp\= -* i S E tC-Vl \l\A-np\ (V)I Pi"11 J
The power per milliradian of horizontal arc is obtained bydividing (?) or (VI by 2itxI0'.
, = — - JL / IX)V p
17
JO1
o 1 0 "
10"
GlyJ « 2.1 y1/3 y « 1• G,(y) « 1.35 y'Afa y » 1
10"4 10"3 10"2 10"1 10° 101
y« y x - w/«e
| i o u
\SURF
^——-
NSLS\•VUV
NS15\ \XRAY \ \
\ \ \
\ . \ \
I 101 102 103 10* 10s 108
Ene«jy
18
Helical Undiitalor*1'
1. Idealized Field
«*= By Kos(*y :)!*•» sm(*i/ .•) y")
2. Kealislic Field
.1. Kleclrun Urbll In Idealized Field
-COS(i(;l
4. Radiated Wavelength
Me A c !
S. Spectral and Angular Distribution (Forward Dir.)
<W _ laNJ-fK2 J_ _AOJ sin;(../2)
<"J ( I + Z f 2 ) 2 ' «» U/2)2
with units of [pholons/scc/sKradianl. I in Amp, c=l 6 x ! ( r " C . a= 1/I37.W and x = 2xNu«i> - o>,)/(0r. The spectrum is cen-lered about <or = 2c<t(. yVC 1 + ^ 2 ) with n (FWHM) lincwidlh of
lianar Undulilor*'•'*''
I. Idealized Kit-Id
II1 = Ituiiv.ili :) i"
1. Realistic Kicld
II, - I I .
/(v = A(/cosli(t(.vK°«Mif : ) . ".. " -"j MIIIU*/ > IMIII*,
.V KkTtrmi (Irl)it In Idculi/ed Held
4. Kudlalfd WaX,. . • « ,
5. Spectra I and Aujiular Distribution (IWwunl S»ir.)
" i l C CO ( t n :2l
with units of [phutons/scc/steruitian). I MI Amp, v - 1 <>' K) ' ' <
where n = 1.3.5 a = I/I37.H4 and
=I.) flV,
h. Central four Radiation Opening Angle
Using this definition of ihc radiation opening angle Ihc spec-irai and angular dislrihution in ihc forward direction at to = (0n
can be rewritten as
7. On AxK feak HriKhtness At u> = co.
«„ = •
where 1, , = \ o , ! v •
N. Optimum K«ta & Dispersion Function In Insertion
<>. Total Power Radiated
3X.7.26C2(GrVl/
(cm I
0.45
0.30
0.15
0
• /:V&• 1 '/•' \ N%>
III ^Us-
— n=1— n=3—.- n=5 -— n=7
-
0 2 4 6K
8 10
Ptamr
For K > 1 an insertion is called a wigglcr. 'I'IK' prn[xTin^of wigglcr radiation are akin to those of are sources. The critk;ilenergy or Ihc photons depends on ihc angle of observation.
r vn
The flux and toul power radiated arc given by.
Flux = 2Nwxl.arc source flux of same c r ) .
7.26 E2lGeV] l\Amp\ Nw K'Pr{W\=-
(cm]
Permanent Magnet Undulator Field VtnmG*?1"'*'3
1. Pure SmCo,
where g is ihe gap of the undulator.
2. Hybrid llnduljtors
fl0 {7-) = 0.95 a exp
where a, b and c are given in Table I for Iwo types of materialswith the restriction, 0.07 S f lXv S 0.7 .
Parameterabc
SmCo,
3.M5.47I.H
Nd-ft-B3.445.081.54
Table 1
r
Effects of Planar Insertions on Ihe Ring
I.) No Net Deflection or Displacement of c~ Beam Requires:1/2
- L • • •
2.) Betatron Tune Shift. Av:
.1.) Maximum Distortion of the (1 Functions, A(V(i:
AP. () aft, 2nAv,()
Pi ~ P,. ~ sin(2nvv)4.) Efl'ect of Wij!glers & Unduhitors on the Energy Spread, ar:
I + r— I +
KKr KrS.) Rffect of Damping Wipglers on the Emiltancc. r:
2V2n'p>'1<^/H.>
f I f t/T 7 1 i' where <HWJ>> = — f - ^ - [ n + (pn 1*11)*]. subscrinis
C ' p 2'M,U,O' denote wig^lcrs, undulators & dipoles respectively and C
^ is (lie ring circumference. References: Hoi , Ka2. Wi l .
24
Synchrotron U(hl Sources Worldwide
Kin* Location Stilus E |GeV| X, |A]
BRAZILI.NLS
KKANCEACOSUPERACODC!ESRF
(iERMANYCOSYBESSY 1KSSQBESSY 11DORIS
ITALYADONEELETTRA
JAPANSORNTT-llNIJI-llUVSORAURORALUNANTT-ITERASSORTECtHISORPH.FACT.
Campinas
Or sayOrsayOrsayGrenoble
BESSYBESSYKFKBESSYDESY
RomeTncslc
Tokyo Univ.AisugiTsukubaIMSSHITsukubaAuugiETLTsukubaHjro&himaKEK
D. UC
1)D
r>D. UC
15, UCDD. PLD. PLP
PD. UC
DD. UCD. UCDD. UCD. UCD. UCDD, UCD. PLD
2
.54s
1X56
.6
.K1.21.55.
1 5t
.38
.55
.66.65.X.8.8
1.01 52.5
18.6.1.4
.6.1.3
I I I19.42.3fij
.55
8 J3..S
11216.8.16.25710.221.820.221.8156
1 1
6GeVTRISTAN ARTRISTAN MR
RIKENKEKKEK
D. PLPP. PL
PEOPLE'S REPUBLIC OF CHINAHESYRLBEHC
HefciBeijing
SOUTH KOREAPLS
SWEDENMAX
TAIWANSRRC
Pohang
Lund
Taipei
UNITED K INGDOMHELIOSSRS
USASURF IISXLS
vuvALADDINCAMDALSXRAYSPEARCHESSAPSPEP
USSRSIBERIA I
Oxford Ins.Darcsbury
NBSNSLSNSLSWisconsinLSULBLNSLSSSRLCornellANLSLAC
Kurchatov
D, UCP
D. PL
D
D, PL
D. UCD
DD, UCDDD. PLD. UCDDPD, PLP. PL
D
6.6.5
10.
.»2.X
2.
.55
1.3
.72.
.3
.7
.75
.81 21.52.53.5.7.8.
.45
.648
1.38
24.32.6
3.8
42.8
8.9
H.I3.V
1739.8
2522.7
9.58.12.52.61.5.64
1.8
VEPP2MS60SIRHISYPI 1VEPP3SIBERIA IIARUSVEPP4
D= DedicatedPL= Planned
NovosibirskMoscowTomskYerevanNovosibirskKurchalovYerevanNovosibirsk
P--: Pan
DPPD. PLDDPD
uitic
.67
.681.361.82.22.54.56.25
UC= Under Consiniciion
35.29.4.1.24.21.81.0
Light Swrcc UnicesThe following pages contain a picture of ilic camiimu) lama-
for many nf the existing ami planned synchrotron lijilil MIIIKVSA MAD"' data set fur t\H'h ring is UIMI incliutdt. IV- M'MupuU'Aircnglhs and locations arc included where known.
The symbols and units arc as follows:
SymbolE I Energy
Nunihcr of Suporpcrirxls
K,
Physical Quantity I Units
Horizontal Beliitrnn TUIH%
Vertical Beiairnii TttiKMomentum CompactionEmiiianccNatural Honiontal ChrouuticityNatural Vertical ChrtHitaticity
- a-ll
111 C.I.I
N M no p
s I "1 0
to O
" m o*- - I £* s* s i s
t n
MACHINE FUNCTIONS [m]
cn_» _» toO en O
•
1 • 1 T
TITLE. "SURF II"! :FieId Index, n= .59, one 360 degrees dipolc! :B= 1.2 Tesl«, rho «.I3.1 m! .DATA COURTESY OF R. MADDEN AT NBSB :SBEND,L=5.2359«JCI=.J4%,ANGIi;=T\VOI'lHSUP :LINE=(B)USE.HSUPPRINT,#S/ETWISS.TAPESTOP
TITLE, "SUMITOMO AURORA"! :Fic1d Index, n* .25, one 360 degrees ilipoleI :N. Ttkahuhi. NIM B24C5 p. 425 (IW7).B :SBEND,L=P1.KI=I..ANGLE=TWOPIHSUP :LINE=(B)USE.HSUPPRINT,#S/ETWISS.TAPESTOP
Propenies of Weak Focusing Rings in t -'-A—
, = VT-n v, = Vn p, = -r£— (1, = -liV I - n \n
a, = av = 0 $, = - - "' *"' 4, = -J--
Ien
MACHINE FUNCTIONS [m]o en o u» o
TITLE, "SOR RING, TOKYO"' DATA COURTESY 01' Y. KAMIYA A I KI-.K. Jl'NI: IWK01' :(HMDRUPOLE. L=.l. KI =(>.(IK(iy 17X<,QD :OUADRUPOLE.L=.I.KI=ftJ-<52^2:110 :SBEND,L=.K6.W37.KI=-.37l«)(X)K.AN(il.l-:=TWOIM/K.I) I :DRIKr.I.=.65.<i1)2 :DRIIT.L=O25in :DRIKT.I.=.I.1IISUI' :LINE=(l)I.B0,U2.yrII.SK.HSIJP,SYMM.SIII>EK=4l'RINT.#Sfl-TWISSST01'
ACO - FEL OPTICS
0 1 2 3 4
DISTANCE [m]
E= 0.536 a- .417E-01
Nf« 4 £- .192E-O6
IM« 2.816 fx- -3.56
v - 1.631 t* -8.79
5 6
— 10,,
3.1
TITLE, "ACO FEL OPTICS"! : M. SOMMER, BNL REPORT 51959. P. 114 (1985).Ql :QUADRUPOLE, L=.33. K 1=6.53807350Q2 :QUADRUPOLE. L=.154,KI=-8.4329I8BD :SBEND,L=.871792,KI=-.405811,ANGLE=.78539B1SP :MULT1POLE,K2L=0.SD :MULT1POLE,K2L=0.131 :DRIFT.L=.94D2 :DR!FT,L=.27D3 :DR1FT,L=.!83HSUP :L!NE=(DI,BD,D2.QI,D3.Q2,O2.D3,QI,D2,BD,l)l)USE,HSUP,SUPER=4PR1NT.#S/ETW1SSSTOP
MAX - LUND
3 6DISTANCE [m]
0.550 a- .198E-01
N,« 4
vx- 3.152
v 1.323
£- .796E-07
**" ~4'07
TITLE, "MAX"! DATA COURTESY OF M. ERIKSSON AT l.UNI)
Q2QiHI)SFSO01020.1HSUP
:QUADRUPOLE. L=.2. Kl=4.42:QU ADRUP0LE,L=.2,K 1=3.14:QUADRUP0LE.L=.2,K 1 =4.35:RBEND.l.=l.,ANGLE=TWOl'l/H,
:MULTIFOLE,K2L=0.:MUI.T[POLE,K2L=0.:DRIPT,L=I.3:DRIFT,L=.275:DRir-T,L=,657
:l.INE=(Dl,01.D2.y2.l32.HO.O.1.0:lUSE,HSUI'.SYMM,SUPKR=4
: • PRINT.KS/ETW1SSSTOP
IMS UVSOR
2.5 5.0 7.5 10.0 12.5 15.(1OISTANCE [m]
0.600
4
3.250
2.750
o - .298E-01
€ - .70OE-O7
( ( - -5.08
f - -4.75
TITLE,, "UVSOR"! DATA COURTESY OP Y. KAMIYA AT KCKQi02Q3Q«BDSFsnDlD2D3D4D5D6HSUP
:QUADRUPOLE, U .2 , KI=3.3K4OS:QUADRUPOI.E,L=.2,K 1=3.62)5:QUADRUP0LE,L=.2,K 1=2.92:QUADRUPOLE.L=.'),KI=2.7:SBEND.L=1.72787S9.ANGI.[r.=.7XM<)KI
:MULTIPOLE,K2L=0:MULTIPOLE,K2L=0.:DRIFT,U1.232:DRIFT,L=.5:DRIFT,U.45:DRIFT,l-=.5.li• D R I K T ! U . 5 2
:DRIFT,L=,435:LINE=(DI,D2,Ql,D.1,Q2,lM.I»li,n.S.gvnfi.l)(i,<J.|,|)(
D6,QJ,D5,BI),D4 02.1)3.01,132,1)1 >USE.HSUP,SUPER=4PR1NT.#S/ETWISSSTOP
20
I1 5
2 10
5
0
-5
NSIS VUV
2
A
i \
UV
/»\\\\
n J-u c-
//
•> /
> /
\i
11/ \
/ >
""" n
•
\\\
i ,•
A/ \_,/ '
** •
. ' >*
VIf
[ /
' \ n—3 u
0 2.5 5.0 7.5 10.0 12.5 15.01
DISTANCE [m] j
E* 0.744 a - .235E-01 10??
Nt« 4 £• .138E-06 — • f [
3.123 ,- -3.50
v- 1-179 (y - -5.00
TITLE. 'NSLS V U V! DATA COURTESY OF G. VlCiNOLA AT HNl.Q1 :QU ADRUPOLE.L=.3,K 1 = 1.80943467Q2 :QUADRUPOLE,L=.3,KI=1.120912Q3 :QUADRUPOLE,L=.3,Kl = I.K7<)7(>l'iHD :RBEND.L=1.5.K1 = -.O267S4l85.ANGl.f:.=.7K<WXlHSl: :SEXTUPOLE.L=0..K2=<>.SL) :SEXTUPOLK,l.=0..K2={l.1)1 :DRIIT.1.= 1.62KD2 :DRIFT.L=.351)3 :DRII-T.L=.65D4 :DR1FT,L=.41D5 :1)R1FT,L=.59HSUH :[.INE=(DI,QI.O2.O2.llSE,HSlJP.SYMM.SUI'nR=4PR1NT.KS/ETWISSSTOP
BESSY METRO
0 2.5 5i.O 7.5 10.0 12.5 15.0 17.3
DISTANCE [m] |
E-
N ."
•7
0.800
4
5.648
2.248
a*
€"•
*„«
.121E-01
-10.83
-8.63
—r«
41
SETOPTS, ECHO, -SYNCHTITLE. BESSY METRO OPTICS! DATA COURTESY OF B. SIMON AT BESSYDQU1 :QU ADRUPOLEA=.44.K 1 =-1.89315DQU2:QU ADRUPOLE,L=.44,K I=+3.OI445AQUI :QUADRUPOLE4J=.44,KI=+3.37020AQ.U2:QUADRUPOLE,L=.44,K1=-I.62679SXI :SEXTUPOLE,L=.25,K2=0SFI :SEXTUPOLE,L=.25.K2=67.6973SDI :SEXTUPOLE,L=.25.K2=-32.02.<i2DDRO.DRIFT,L=1.634DDRI:DRIFT,L=.25DDR2:DR1FT,U.835DSXA:DR1FT.U.I2DSXB:DR1FT,L=.46SADRI:DRIFT,L=.B35ADR2:DRIFT,L=.25ADR3:DRIFT,L=.835HB:SBEND,L=.9341 ,ANGLE=.5235987,EI =. 1726682,E2=. 1726682. &
HGAP=0.03,FINT=-1.2888046DOU:UNE=(DDR0,DQU I .DDR 1 .DQU2.DSXA.SX 1 .DSXB)ACH:L1NE=(HB.DSXB.SF1.DSXA.AQUI.ADR2,AQU2,ADR3,HB,&
DSXB.SD1,DSXA.AQU2,ADR2,AQUI.ADRI,HB)BI :LINE=(DOU,ACH.-DOU)USE.B1.SUPER=4PRINT.#S/ETWISS.TAPESTOP
42
ETLTERAS
2
0.800
4
2.250
1.250
4 6 8DISTANCE [m]
c-
*,-
.122E+00 — 10TJ>
.555E-06 - — f
-3.15
-3.30
L
TITLE, TERAS"! DATA COURTESY OFT. TOMIMASl 'AT I . I . I l l I.AIiQl KJUADRUPOLE, L=.2. KI=4.WV.(HS(iQ2 :QUADRUPOLE. L=.2.KI=-S.-1SISSHD :SBEND,L=l.5707<*6.1.KI=<I..AN(il.l.--.7S5.WSIA
EI=.2W2.E2=.2(M2SF :MULTIPOLE.K2I.=<).SD :MULTIPCH.E,K21.=().L>l :WIFT.L=.9D2 :DRIFT,l.=.4-45D.1 :DKIFT,U.7ISIISUP :LINE=(USE,HSUP,SUPER=»PRINT.KS/ETW1SSSTOP
25
15 •
HEFEI
LU
I
-5
1 1 1
\
I1111
>A
- -•- \ y ,n JJ*< ,?f
u * — • I
i i i
* i
/ ;
A\J HX /*-'
•
iii
iij
i /
&T
1 *!M(1
!\Mi \i \
• \
n N.
0 2.5 5.0 7.5 10.0 12.5 15.0 17.9DISTANCE [m] J
E* 0.800 a= .128E-01 — 10f)i
N§- -2 «- .274E-07 - — ^ j
vx- 5.822 (x- -17.38 (
v * 2.420 f - -6.92
45
TITLE. HESYRL HBLS'! DATA COURTESY OF H. DUOHUI AT HESYRLQl :QUADRUPOLE, L=.3. KI = 2.494447Q2 :QUADRUPOLE, L=.3. KI=-2 .526518Q3 :QUADRUPOLE. L=3. K\= 3.820103Q4 :QUADRUPOLE, L=3, Kl=-.7476705 :QUADRUPOLE. L=.3, Kl=-3.107723Qft ^UADRUPOLE, L=.3, K l= 4.R2I645Q7 :QUADRUPOLE, L=.3, K1= 4.633252QX :QUADRUPOLE, l.=.3, KI=-2.76564B :RBEND, L=1.I635. ANGLE= TWOP1/I2.SF :SEXTUPOLE, L=0.. K2=0.SD :SEXTUPOLE. L=()., K2=0.DL iDRIFT, UI.68IIDQ :DRIFT. [.= .32DBQ :DRIFT. L=l.DSB :DKIFT, L= .72IX)S :DR!FT, L= .28
HSUP :LINE= (DL.QI.DQ.Q2.DI)Q.B,DSB,SF.DQS.&Q3.DQ,Q4.IX!S.SD,DSB.&D.DSB.SD.DQS.Q5.DQ.Q6.DQS.&SF.DSB.B.DBQ.Q7,DQ.Q8.DL)
RING :LINE= (HSUP.-HSUP.HSUP.HSUP)USE. RINGPRINT. #S/0TW1SSSTOP
25
20
| 15
I 10g 5LU
i 0
-10 h
SRC ALADDIN
5 10 15DISTANCE [m ]
0.800 a« .339E-01
'»" 7 l 1 3 2
'..« 7.237
e- .976E-07
fx- -11.93
fy« -23.80
JIjiji
*•' « A1)/ 1 ' ' / i
/ l i :' ( / k '-•'' i y» ' / A" ' / i y /1I i//,^/ ft
" ~ kr h • AJ
• • ,
iji'i
/I •IV '
/ r 'J \\ i
20 25
47
TITLE, "ALADDIN"! ALADDIN DATA COURTESY OF I. HSU AT SRCQlQ2Q3Q405BDSFSDDlD2D3D4D5D6D7D8D9D10DllFSUP
RING
:QUADRUPOLE,L=.25,KI=4.65I721:QUADRUPOLE,L=.25,KI=-5.566506:QUADRUPOLE,L=.2S,KI=4.6S!2208:QUADRUPOLE,L=.25,KI=5.31 3864:QUADRUPOLE,L=.25,KI=-5.614159:RBEND,U1.O9O83>NGLE=.5235987:SEXTUPOLE,L=.0,K2=0.:SEXTUPOLE.L=.0,K2=*.:DRIFT,L=0.2:DRI[-T,L=.449:DR1FT.L=.873:DR1FT.U1.73:DRIFT,L=.2.1:DR1FT.L=.5:DR1FT,L=I.55:DRIFT.L=.2:DRIFT,L=.3:DRIFT.L=I.8.1:DRIFT,L=2.:LINE=(DU.Q1,D2,Q2.D3.Q3.D4.Q4.D5,Q5.D6,BD.&
D7.SF.D8,Q4,DS.Q5.D 1 .SD.D9.BD.D7.SF.&D8,Q4.D5,Q5.Dl.SD.D9.BD.D10.O3.D3.Q2,D2.&Q1.D11)
:LINE=(4*FSUP)USE.RINGPRINT,#S/ETW1SSSTOP
MACHINE FUNCTIONS [m]
« « - ; - T "a
l
7 -7 - I
Ien
o h
en
enMO
-
-
1V
\
l"III»^
i
- ~ ; ^ —
i
•i
i.i
• « — _
I
1
-
iiii
-----
CO
49
TITLE, "SUPERACO"! : M. SOMMER, BNL REPORT 51959, P. 188 (1985).Ql :QUADRUPOLE, L=.4, K1 »• 1.4753974Q2 :QUADRUPOLE,L=.4,K I =2.79922985Q3 :QUADRUPOLE,L=.4,K 1=2.70282392Q* :QUADRUPOLE,L=.4,K I =-1.47539743BD :RBEND,L= 1.335177, ANGLE=.7853981SF :MULT1POLE.K2L=0,SD :MULTIPOl.E,K2L=0.D1 :DRirT,L= 1.785D2 :DR1FT,L=.35D3 :DRIFT,L=.9HSUP :LINE=(D1.Q1,IJ2,Q2,D3,BD,D3,Q3,D2.Q4,DI, &
Dl ,Q4,D2,Q3.D3,BD,D3,Q2,D2,Q 1,01)USE,HSUP,SUPER=4PRINT.#S/ETWISSSTOP
so
LSU CAMD - PREUMINARY DESIGN
20
15
y 10
-5
\i \
' \
0 2.5 5.0 7.5 10.0 12.5 15.0DISTANCE [m]
E- 1.200 « - .347E-01 10tj.
V
4
3.259
1.168
.211E-06
-4.52
-3.79
riTL.l.. "LSI! CAMl) - PRELIMINARY1 DESIGN"DATA COURTESY 0 l r B. CRAIT A T CAMB-I-SU
1)11)2D<IM1)5DOQAonorSI)SFBUND
: DRIFT,:DR»T.DRIH.:DRIFT.:DRIIT.iDRIFV.:QUAD.:QI)A1),QUAD.
:SliXT.
.= l.d
.=0.25.=0.fi.-0.21.=(>..!l.=O..l!.=(). 1.=0.1,
:.SEXT. L=<).l.:RUEN1). U 2
IIAFSUP :LIN1£=(DI,C
K\- +2.001.WlKl= I.Sd.WKd
5. Kl= +2.X.M.l';(iK2=-25.JIWIK2=«I7.14186J.ANfil.l:=TWOI1l/»..KI=()A,D2.QH,I).USF.NI),D4.SD.
USU.HAPSUI\SllHliR=4,SYMPRINT.HS/9ETWISSSTOP
20
15
10
5
0
lIt| lM1 11 11 1
— * ^ *
(' I
' \ ' \<- t \i i
u u*-
1 . 1
TAIWAN SRRC
» •\ f\ A A .'
\ i
i
: \i
<i r—'U
i
J
u
0 5 10 15DISTANCE [m]
E- 1.300 a- .678E-02 -
v- 7.175
¥' 4.125
€- .194E-07
f^- -15.61
t~ -7.61
20
X
TITLE. "TAIWAN SRRC"! DATA FROM SRRC STATUS REPORT JAN01Q2Q304BO
SDDlD2D3D4D5D6D7DRFSUI>
:QUADRUPOLE. L=.3S. KI=-l.500H*W:QUADRllPOLE.L=.3S.Kl=2.833li5l5<J:QUADRUPOU-.L=.3S.KI=-.75801M5H:QUADRUPOLE.L=.3S,K I=2.73(W426:RBEND,L=l.219985.ANGl.n=TWOPI/l8..KU
:SEXTUPOLE,L=.I.K2=0.
RINGUSE.RINGPRINTJS/ETWISSSTOP
:DRIFT.L=3.DRIFT,L=.3
:DR1FT,U.595:DRIIT,L=.325:DRIFT.L=.335:DRIFT.L=.5H5:DR1FT,L=.!5:DR1FT.L=I.28
:LINE=(Di,QI.D2.O2,D3.Q3,D4.BD.D5.SD.D6.Q4.B7.SF, &D8,BD.D8,Sr-,D7.Q4.D6.SD.D5.BD.D4.Q3.&D3.Q2,D2.Q1.DI)
:LINE=(6'FSUP)
MACHINE FUNCTIONS [m]
TITI.I-. "AUONE"! DATA COURTESY OF M.PRI-Ol-R AT INIrN0I r :QUADRUPOI.K. L=.5.12, KI=.T)M>M(11 > :QV ADRUPOLE.U.5M.K U • .781347IU5 :SBEND.1131 :DRIFT.L=I.293112 :DRIFT,I.=.2%W :DRI»=T.L=.41HSUP :UINP.=<ni.QI:,USK.HSUI'.SUI'ER^UI'RINT.«SA:TW1SSSTOP
FUNC
TIOIN
E
Q3
25
20
15
10
5
0
«;
LBL -l i t *
1 *
• - - • ' • '
i t; i
\
iiiiiii
» A \
n p/n p?
i » i i
ALS•
hj
iiiiiijiiii
/rt&?\ 1
i
ttii
V"n
u
i i
0 2.5 5.0 7.5 10.0 12.5 15.0 17.1DISTANCE [m] |
E- 1.500 a* .159E-02 10»
H> 12
14.266
8.184
e- .340E-08
t* -24.52
t • -27.90
57
TITLE. "ALS"! DATA COURTESY OF A. JACKSON AT LBL
01Q2Q3
BDSFSDDlD2D3D4D5D6D7DXD9DIGDllFSUP
RING
.QIMDRUPOLE, L=.35. KI=2.1908<W:QU ADRUPOLE,L=.2.K 1 =-2.051427:QUADRUPOLE,L-.5,K 1 =2.620561:QUADRUPOLE,L=2.K 1 =0.:RBEND,L=.«542I,ANGLE=TWOPI/36.,KI=-.8I947:SEXTUPOLE,L=.0,K2=O..SEXTllPOLE,L=.0,K2=O.:DRIFT,L=3.37S58S:DRlFT,t,=.425:DRIFT,L=.3477:DRIFT,L=.4:DRIFT.L=.3227DRIFT,L=7:DR1FT,L=.2:DRIFT,L=325:DRIFT.L=.3:DRIFT,L=.2727:DRIFT,L=.4:LINE=(D1.Q1.D2,Q2,D3.BD.D5,SD,D4,Q3,D7,SF.D8,4
O4.DI0.BD.&D10.Q4.D8.SF.D7.Q3.D4.SD.D.'i,BaD3.Q2,D2,Ql ,D 1)
:LINE=(12"FSUP)USE.RINGPRINT,»S/ETWISSSTOP
25
^ 2 0
£ 15o
hI 5
-5
BESSY II - PRELIMINARY DESIGN1
* •
n'———•*• v
1* 1(|
/
nu
i
• • i
•>.
1 ii\\\ii
it
, V\•hfrArS-,|J I—IT— -JJ-LJ-^
• . 1
1I
1
A/
ii
ii \ 'i
< if
!<ili1 v/ \ "
M n
•u 'u
5 10 15
DISTANCE [m]
1.500 a- .205E-02 —
10
12.180
7.280
c- .882E-O8
fx« -23.71
t * -21.21
20
sirroiTS, ECHO, SYNCHTITLE. UESSY II! BESSY II DATA COURTESY OF li. SIMON AT BESSYPARAMETER.PI=3. 14 I W27PARAMETER.NSUPER=IOPARAMETER,WIEVEL=3.PARAMETER,ANZAIII.=NSUPl:K*WII-VEI.QI:QUADRUPOl.i:.L=.4.K I -0..10-WQI:QUADRUK)LE.1.=.4.KI=2.3I3SSQ.l:QUADRUP01.K.t=.4,KI=-2.IWWiQ4:QUADRUI'Ol.E.I.=.4,KI=3.051)lQS:QU AURUPOI.i:.l.=.4.K I =• 1.4176
Sl>l:SEXTUPOLE.I.= .2.K2=<)DI:[>Rin'.L=2.6
D4:BRIFT.I.= ..1DS:DRIFT.L=.2D6:DRIFT.L=.SU7:DRIFT.1.= 2
I»:DRIFT,L=.7D10:DRIFr,L=l.3HBl:SBEND,L=.4.ANaLE=PI/ANZAHL.EI=PI/ANZAHL,E2=<)HB2:SBEND.L=.4.ANGLE=PI/ANZAHL.E1=O.E2=P1/ANZAHL1S:LINE=(D I ,Q I ,D2.Q2.D3,Q3,I34,HB I)ISM:LINE=(HB2,D4.Q3.D3.Q2.D2,Ql.DhDS2:LlNE=(HB2.D5.SDl.D6.Sf:l,lJ7,Q4,D«.QS.D9.HBI)DSM2:UNE=(HB2.D9,Q5.D8,Q4.D7.SFI.D6.SDI,D5.HBI)FULLC:LINE=(1S.DS2.DSM2,ISM)FULL:LINE=( 10*FULLC)USE.FULLC.SUPER=10PR1NT.#S/ETWISS.TAPESTOP
ILU
30
25
20
15
10
0
HiSOR1 1 1
1
'. Ir 1' \
1
1
*
- ' ' u »^—• '
- HIROSHIMA• § i i i
(i ,ii <i i i/ tii il.' i'
/ i.' li
A ' "/ \ ' iv/ \ / i -
/ \ A /
0 2.5 5.0 7.5 10.0 12.5 15.0 17.5DISTANCE [m]
E- 1.500 a« .118E-01 10ij|
Ng- 6 e- .828E-07 —- (?
vx- 5.250 fx- -11.01
» - 2.250 f - -7.75
61
TITLE. "HiSOR - HIROSHIMA"< OATA COURTESY OF Y. KAMIYA AT KKK
Q2y inosrsn01112D.I04OSHSUP
iQUADRUPOLE. L=.4, KM.2D692MI3:QV ADRUPOLE.U.4.K 1 =-1.3936996:QUADRUPOLE,L*.4,KI=I.86385992:SBEND,L=2.I8.ANOLE=TWOPI/I2.
:MUI.TIP0LE,K2L=fl.:MULTIPOLE.K2L=().:I)RII-T.L=2.37S:ORIFT.L=.62S:ORIIT.L=.65:ORIFT,L=.25:DRIFT,L=I.
:l.lNE=(DI,QI.D2.Q2.D3,nO,l>»,.SO,D5.SI:,O4,Q3,&O4,SF.D5.SD,D4.BO,D3.Q2,D2.QI.DI)
PRINT.*S/ETWISSSTOP
MACHINE FUNCTIONS [mj
D O O O O O
TITLE, "DC1"! DATA COURTESY OF J. LEDUFF AT LURE! DEFINITIONS DES ELEMENTS1:>1:DR1FT,L=2.<WD2:DR!FTA=1.«77I)3:DRIFr.L=0.465
D5:DR|FT,L=«..W.<iDh:nRIIT,l.iO.528l57:nRlFT,L=0.456
QFI:QUAD.L=«.526,KI = I.22S8OJ32.0UA»X=0.494.K 1 =• 1.2.1 I<WOWQUAD.I.=<).247.KI =1.301QIM:QUAD.L=<>.494,KI=-0.542Sgi:5:QUAD.L=().247.KI = I.S767QDfi:gUAD.L=<).247.KI=-1.3<XM.l0R:QHAD.I.=<).494.K 1=0.30547BN'D:SBEN1).L=2..ANGLI;=+(1.52.16AY:SBEND.L=0.72,ANOLE=O.I745,TII-T.I-2=«.(iS7:.sAV:.SBEND.L=(I.7I.ANGI.I:=-(I.1745.TII.T.SF:SEXT.K2=I.I1.V*SI):SEXT.K2=-2.l5«61i; DEFINITION DE LA DEMI=MAILLEDM:LINE=KDI,AY.D2.gFI.D3.gD2.D4.AV.l)5.BNI).[X).QI-.l.SI'.yi!.&D7.QD4.D6.BND,D6.Q»:5,Sr.QF5.D7.gii6.SO.gi».n(..BN[).OS..V:OF7.D9)USE.DM.SYMM.SUPER=2
TWISS.TAPE.CHROMSTOPEND
64
g
20
15
10
5
0
ELEJTRA
i i
i ii i
i i '
A i\r ,./ vi
.nj.
1 1
- SINCROTRONE TRIESTEl i t
iii t
'» t i
\ '\ i\ i\f\\ i
V x \ '/ r- *•
Mi .nX. n._r" ryi "i—ly [j
i i i
0 5 10 15DISTANCE [m]
E« 2.000 o - .159E-02
N - 12 e- .720E-O8
v= 14.305 fx- -41.11
vy= 8.200 fy= -13.96
20 251
TITLE, "ELETTRA, SINCROTRONE TRIESTE'! DATA COURTESY OF A. WRULICH AT TRIESTEQl .QUADRUPOLE. L=.34. KI =-1.58789
Q2Q3Q4QSBODlD2D3D4D5K.SIS2S3HSUP
FSUPRING
:QUADRUPOLE. L=.5. K 1=2.2453:QUADRUPOLE. L=.34, Kl =-.896051•QUADRUPOLE. U.5. K1 = 1.8O457:QUADRUPOLE. L=.I7. Kl=-1.11814:RBEND,L=1.44,ANGLE=,261799.K l=-.4297:DRIFT,L=3.O76:DRIFT,L=.29:DR1FT,L=.21:DRIFT.L=.475:DRIFT,L=2.094:DR1FT.L=.31:MULTIPOLE,K2L=<).:MULT[POLE,K2L=O.:MULTIPOLE,K2L»0.
:LINE=(D 1 ,Q 1 ,D2,S 1 ,D2,Q2.U3,Q3.D4. &BU.D4,Q4.D2,S2,D5,S3.D6,Q5)
:L1NE=(HSUP.HSUP):LINE=<I2*FSUP)
USE.RINGPRINT.*S/ETW1SSSTOP
POHANG - PREUMINARY DESIGN
20
" 1 5CO
o5 10
-5
0
f \; \• \
" Ji.
/
/ t
- "WLJ
\I)iii-iM1 \
L \Ik »
1
iii
:<1•']
u
/ i.' i
,' i' 1
iit}V
IAl\1 \1 V1 v^
/ * • "
u
0
E«=
N."V*
V*
5
2.000
12
14.295
6.194
10 15DISTANCE M
«- .159E-02
e« .114E-07
(„- "25^4
t~ -19.15
20 25I
— 10,,
:.:.:{; [i
i
TITl.K.POHANCi! 1'OHANG OAT A FROM I'LS TR/BI) XX<*> NAM. I7T. AL01g:Q \Q4QSHI)S10.SFsi)1)11)2D.I1)4
D7DSFSUP
:yUAI)RUI>OLE.L=.4. KI = 1.7487I9:yUADRlJI>OLlU.= .4.KI=-1.545169:QU A [)RUI'()l.E.I.=.4.K 1=1 4W.S27:QHAl)Rlll'OLE.l.= SS.KI = I.KI4I25S
:SE:.\Ti:r<)LIL.I.=.I.K2=<l.:SI-XTUI>OLE.U=.2.K2=«.:S[:XTUPOI.[-:.I.= : .K :=O:DRIKT.l.=3.3:DR1FT.L=.I2:DRIFT.L=.n:1)RIIT.L= 5S:DRIFT.l.=.S:DR1FT,L=22:DRIFT.L=I.X1:DRIFT.L=.3S
RINGUSE.RINGPRINT.#S/ETWISSSTOP
Q3.D6.O4.lW.SF,D7.Q5.l)X.HI).l)X.(}.S.l)7.&SK.D3.O».n6.Q.1.[>3.SI).D5.H[>.l)4.y:.l)3.SRl.&D2.QI.DI)
:LINE=(I2'FSUI'I
15SRS2 - DARESBURY
10CO
o
I 0
-50 1
E- 2.000
n ™ io
v* 6.250
i/= 3.250
2 3 +DISTANCE [m]
««= .289E-01
c- .108E-06
fx- -10.29
* « -5.38
5 6
— 10"»
TITLE. "SRS2 DARESBURY"! DATA COURTESY OF V. SULLER AT DARESBURYQI :QUADRUFOLE,L=.3. K1 =-1.5633944Q: :QUADRUPOLE,L=.5.K I = 1.2782629BD :SBEND.L=2.188001 .ANGLE=TWOP1/16.SF .MULTIPOLE.K2L=0.SD :MULT1POLE.K2L=0.Dl :DR1FT.L=4725D2 :DR1FT,L=2.I67U3 :DR!FT.U.372SFSUl' :LINE=(D1.QI.D2,Q2.D3.BD)USE.FSUP.SUPER=I6PRINT,iS/ETWISSSTOP
70
NSLS XRAY
5 10 15DISTANCE [m]
2.500 a« .654E-02
8
9.144
€- .102E-06
f - -22.37
20 25
Ef6.202 L- -16.50
TITLE. "NSLS XRAY! DATA COURTESY OP C. VICiNOLA AT BNI.01 :QUADRUPOLE.L=.4.<i.K I =-1.501 K657hQ2 :QUADRUPO1.E.L=.8.K I = 1.337.112*03 :OUAI»'JPOLE.L=.4132,Kl = -04 :QUADRUPOLE,L=.225,KI = I.29B :RBEND,L=2.7,KI=-.Q2(>X4XVSl.AN(il.K-.W2<iVVI>xSI' .SEXTUI>OLE.l.=O..K2=().SB :.SF.XTU1>OI.E,U=(I.,K2=<).1)1 :BRIFT.L=2.251)2 : I3RIFT .L= . ( IX5
B3 :l)Rirr,l.= 34KJ
135 :DRIFT.L=.9
HSUP :LINI:=(DI.QI.D2.O2.l33.Q.1.IM.n.l)5.SO.D5.SI:.IXi.04lUSE.HSUP.SYMM.SUPER=XPRINTTWISSSTOP
PHOTON FACTORY - LOW EMITTANCE
10 20 30
DISTANCE [m]
E-= 2.500 a= .160E-01
40 50
-2
8.250
3.250
e* .129E-06
tt~ -12.67
f - -9.11
— 10,,
' U
TITX£. "KEK PHOTON FACTORY LOW EM1TTANCE"! DATA COURTESY OF Y. KAMIYA AT KEKQ1 :QUADRUPOLE, L=75. KI =-.K15324Q2 :OUADRUPOLE.L=.75.K 1 = 1.02.1431Q.I :QUADRUPOLE.L=.5.K I =-1.243955Q4 :QUADRUPOLE.L=I..KI = 1..18I7(N<.Q5 :QUADRUPOLE.L=.fi.K 1 =798753Q6 :QUADRUPOLE.L=.6,Kl = l.<>6133Q7 :QUADRUPOLE.L=.5.KI=.3.'i.173l2QX :OUADRUPOLE.L=.5,KI=-.994I06Q9 :QUADRUPOLE.L=.5.K I =8806592QIO :QUADRUPOI.E,L=.5.K1=.580822KQl I :Q.UADRUP0LE.L=.5.K I =-.4424B72QI2 :QUADRUP0LE,L=.5.K I =.9082836Ql 3 :QUADRUPO1.E.L=.25.K I =.9082836Bl :RBEND.L=1.944076.ANGI.n=TWOI'l/2KSF :SEXTUPOLE.L=.O.K2=*1SD :SEXTUPOLE.U.().K2=0Dl :DKIFT,L=2..'i D2 ORIIT.1.= IK1)3 :DRIKT.L= 1.735 EM :DRIFT.L=.72SD6 :DR1FT.L=4 23D7 :DRIFT.L=I.O75D9 :DRIFT.L=2IDIO :DRIFT.L=19Dl 1 :DRIFT.L=3.56012 :DRIFT.L=.925DI3 :DRIFT.L=.735HSUP :LINE=(D 1 ,Q I .D2.Q2.D3.B 1 .D4.Q3.D2.Q4.O2.Q3.&
D4.B 1 .D4,Q5.D2,Q6.D6.Q7.D4.B 1 .D7.QX.&D9.SD.D10.Q9.D 11 .SF.D 10.Q 10.D 12.B I .&D13,SD.D1O.Q11.DI2,B1.D13.SF.D1().QI2.&DI2,B1.D12,Q11.D12.B).D13.SF.DIO.QI3)
USE.HSUP.SYMM.SUPER=2PRINT.#S/ETWISSSTOP
IHEP - BEPC
0 10 20 30 40 50
DISTANCE [m]
E- 2.800 a* .206E-01 -
Nf« -2 c- .236E-06 -
kx- 7.24fl fK- -9.35
Y 7-238 ^ - -8.82
70
I-
TITLE. HEPC IHEP BEIJING STORAGE RING"! DATA COURTESY OF S. FANG AT BEPC! HE WARE QUADS & DRIFTS ARE WRITTEN IN 2 COLUMNSQl :QUADRU.L=.6.K1=-.4(I8 Q8 :QUADRU.L=.4.KI = UX)4Q2 :QUADRU.L=.6,Kl=..'i66 Q9 :QUADRU,L=.4,KI=.9IXQ3 :QUADRU.L=.4.KI=.644 QI0 .QUADRUX=.4.KI = I.I7304 :QIJADRU,I.= 4,KI=.8K Qll :QUADRU.L=.4,KI=.9K105 :QIIADRIU.=.4,KI=-.W QI2 :0UAI)Rl),l.=.4.Kl=-.MIQ(> :gilAnKLi.I.=.4.KI = L2K9 QI3 :QUADRU.L=.4.KI = I 32f>Q7 :QUAI)Rl!.l.=.4.KI=-l.(Ki4 014 :QUADRU.U.4,K1= I 171BL :RBEND.L=(l..'i.ANGL[:=.O24O«.<i543Bli :RBEND.L-1.d.ANGLE=.l54671078SF :SEXTU,L=.(I,K2=O.SD :SEXTU.L=.0,K2=().Dl :DRIFT.L=2.5 D8 :DR»;T.L=2..'>5D2 :DRIFT.L=I. D9 :DRIFT.L=.25D3 :DRIFT.L=4. DIO :DRIFT.L=4.25D4 :DRIFT.L=4.2 DM :DRIFT.L=3.ID5 :DRIFT.L=.35 DI2 :DRIFT.L=.68D6 :DRIFT.L=.3 DI3 :DRin\L=.32D7 :DRIFT.L=.65QUAT :LI.NE=(IP1NS.BODY.SPINS)IPINS :LINE=(DI.QI,D2.Q2,D3,Q3.D4,O4)BODY :LINE=(ARCI.ARC2.ARC3.ARC4,ARC?.ARC6.ARC7)ARC I :LINE=(D9.BL.D5.BB,D6)ARC2 :L1NE=(Q5.D 13.SD.D12.BB.D6.O6.D5.SF.D7.BB.D6IARC3 :LINE=(Q7,DI3.SD,D12,BB,D6.Q8.D5,SF.D8>A RC4 :L1NE=(Q7,D 13.SD.DI 2.BB.D6.Q9.D 13.SF.D 12.BB.D6)ARC5 :LINE=(Q7.D13.SD,D12,BB.D6.QI0.DI3.SF.D12.BB.D6)ARC6 :LINE=(Q7.D13.SD.DI2,BB.D5.OI LD10)ARC7 :LINE=(QI2.D6.BB.DI1)SPINS :LINE=(Q13.D6.Q14,D8)USE.QUAT.SUPER=2.SYMMPRINT.KS/ETWISSSTOP
76
SSRL SPEAR
70 •
50 •
I
10 •
-10
-
'}llill
Aiiiiiii\\\
A A
-
K A A / A ,V
0 10 20 30 40 50 60DISTANCE [m]
E- 3.000 a - .417E-01 lOn
- 2
5.256
5.175
€ - .517E-06
{„« -11.32
t • -10.83
" • • $
tH+:v!m*p\.m*v hij>y»j>t!>.*r»»<»w:r
77
TITLE, "SPEAR"! DATA COURTESY OF H. WIEDEMANN AT SSRLQ! :QOADRUPOLE,L=I.O,K1=-.910105
I Q2 :QUADRUPOLE,L=I.34272,KI^,390514Q3 :QUADRUPOLE.L=.5I834,KI=.245597Q4 :QUADRUPOLE,L=.5I834,K1~-.564108Q5 .QIMDRUPOLE,L=.5I834,KI=-.S4979
| Q6 :QUADRUPOLE,L=.5I834,K!=27308I. • Q7 :QUADRUPOLE,L=.5I834,K1=.2985I{. Q8 :QIMDRUPOLE,L=.259I5,KI=-.S37857
B :RBEND,L=2.36825:ANGLE=TWOPI.'34.BHALF :RBEND,L= 1.18413,ANGLE=TWOPi/68.SF :SEXTUPOLE,L=0.0,K2=0.SD :SEXTUPOLE.L=0.0.K2=0.
( Dl :DRIFT.L=1.3448I D2 :DRIFT,L=.85883
D3 :DRIFT,L=6.4I438D4 :DRIFT,U=.6O668D5 :DRIFT,L=2.818451D6 :DRIFT,1^.611269D7 :DRIFT.L=.3O562D8 :DRIFT,IJ=.3O3339D9 :DRIFT,L=2.98163D10 :DRlFTi=l.49O81
. INS :L1NE=(D1,Q1,D2,Q2,D3.Q3.D4,B,D4,B,D5,Q4.D6.&{ BHALFJ)7,SD,D7.Q5,D8,SD.D8.B.D8,SF,D8,Q6,&
L D9)CELL1 :UNE*<Q7,D4.B,D8,SD,D8,Q8)HSUP :UNE=(INS,CELL1.-CELL1,D1OXHO,CELL1,&
-CELL1,D9,CELL1), USE,HSUP,SYMM,SUPER=2! PRINTj TWISS! STOP
78
ESRF
40
UJ
iio
-5
/I\
' 1J 1
. " 1 r—IIII
•n r5^U 'U L -i fl
r
1- x '
I1
I1 S~
•
i1 .—i/\iJ
ji/i
-• \\\Vw
•"nj-fc
1
" • " • »
i
11
//
-1 u1
A
nn1 1i ii iii
;
;
ii
\
n, \1 u
10 15 20DISTANCE [m]
25 30
E-
N."
X
y
6.000
-16
36.200
11.200
« •
c«
{ -
.282E-O3
.695E-08
-114.9
-32.61
T)
TITLE. "ESRF"1 ! DATA COURTESY OF A. ROPF.RT AT ESRF' Qlil :Q.UADRUPOl.E.l.=.4. K l =1 QF1 :QUAnRUPOLE.I.=.«», K l =
QU2 :QUADRUPOUi.L=.5. K l =QD3 ;QUAI)RUPOLE,L=,4, KI=-.<QF2 :QUADRUPOl.E,l.=.5. KI=.7S'«H)3
I Q134 :QUADRUPOl.E.L=.5, KI=-.77O77¥I QF3 :QUADRDI1OI.E.L=.9. KI=.XIlM97[•••• QD5 :QUADRUPOl.E,L=4. KI=-.547HW
Ml :SUEND.L=2.IS728.ANOLE=.(»2324.ni=TWOPI/l2S..E2=.<M.1237M2 :SHI:NO.L=.2927IO,ANGI.E=.(K)5K5,E!=-.IM32.W,E2=T\V()PI/I2»M3 :SBENUL=.29271().ANCLn=.<X)5SS.ni=TWOI'l/l2S..I:.:=-.()43:37
, SF1 :MULTIPOLE.K2L=2.MW9G9E+II SF2 :MULTIPOLE.K2L=2.M8I036E+I
SF3 :MULTIIJOLE,K2L=2.*.31031>E+ISUI :MULTIPOLE.K2L=-.2260ISE+It2.SD2 :MULTIPOl.E.K2L=-.!()775hE+l»2.SD3 :MULTIPOLE.K2L=-.I77S12E+I*2.Dl :DR1FT.L=3.I696D2 :DRIFTX=.35D) :DRIFT.L=4D4 :DR1FT,L= 1.07225t>5 :DRIFT.L=I.O7175
( D6 :DRIFTX=.43, D7 :I3RIFr.L=.5
HSUP :LINE=(D1.0DI.D2.SFI.D2.QFt.D3.Sl)l.l)2.QU2.IM.AI:MI,M2,D5,QD3.D2,SD3,D6.OF2.D7.SF3.t)7,yi:2.«:D6.SD3.D2.QD3,D5.M3.M4.D4.QD4.D2.SD2.O3.&QF3.D2,SF2.D2,QD5.D1)
! USE.HSUP,SYMM.SUPER=I6I PRINT.#S/EI TWISS
STOP
30
25
20
15
10
5
0
_«;
RIKENi *
-
-
/ | i— — — 11
ut
i\M1 1
1
\
n.uf u
- PREUMINARYi
1
\fi,
i
• i
{V . '
DESIGN
-
i'
J ./
.nU 'U
0 5 10 15 20DISTANCE [m]
E- 6.000 a - .186E-03
Nf« 36 e- .823E-08
vt- 32.220 fx- -67.89
v* 11.160 ( - -28.84
25 30
-Y,
TIT! I.. RIKEN 6«i:V FKELIMINARY DE-SUiN"DATA COURTESY OP Y. KAMIYA AT KEiK
y i OUADRUPCH.F.. L=.S. KI=-.ISO321y : .•OUAI»UPOLK.I.=.<».KI=.44I<M:y ! :ytlAtJRUPOU:.I.= 5.KI= 4<W7y-J 0UAE)Rl)E'Ol.[U.= 5.K I =.4.1(119.1y i yuA»Riipoi.F..L=..'i.Ki=.(i(i64:41)1 SBI:.NI).l.=:.IK,ANril.[;=TWOI'l/72SI- :SEXTl.1llOl.n.L=.«.K2=0.si) .si3cn!K)Ui.i.=.(i,K2=.n1)1 .l»ll-T.l.=.1.SD: DRIIT.I.= 4:
01 :D«|fT.l.= l.tD5 :DRIFr.l.=.21)6 :DRIFT.L=51)7 :DRIFT,I.=.4IIS(!I> :LINH=<I>1.QI.D2.SD.D2.Q2.D2.SI:.IJ2.&
D7.D.'i.SF.D.<i.D7.y.'i.E)6.DS..SK)l.sr:.HSUP.SYMM.SUPER=.16PRINT.aS/ETWISSSTOP
82
25
^ . 2 0
ANL APS
15 •
-5
1 \1 \1 1' ! 'i * /•
- • * • * ' / • '
v \ \\\n r»
u u n —
ftt \
/ \1iIn
1
-h-ir
>l1II\
\
•fir.IT
\
<
'y I
»
Jltf
,1
1 t1 1
•
/ ' * ' • • • •
V
u
5 10 15 20DISTANCE [m]
7.000 a - .237E-03
40 £ - .811E-08
25 30
v- 35.205
v 14.310
fM- -63.62
?/= -25.95
TITLIi. "ARliONNH ACS"< DATA COUKTl-SY ()t: S. KKAMhK AT AMQl iQUAORlll'Ol.i;, L=.S. Kl= 4M.W1
Q.I :yi)AI>RUI>(>L.IU-=.5.KU-.4VmxQ4
111 iRHIiNn.l.-V51 :SI-XTUIf)l.l:.l.= .24.K2=(l.52 •Sl-XTUI'Ol.l-:.l.=.24.K2=.(»S:i :Si;XltU'()l.i:.L=.24.K2=.OS4 :S|-:XTUIH)l.l:.l.-.I2.K2=.O1)1 :l)RII'r.l.=1.l
D3 1)RIFT.1.=.11D4 ORIIT.1.= 7(IIS :DRIFT.1.= 2D6 :DRI1T.U.7137 :nRHT.l.= .17I3K DKI1T.U :ii isi i i ' i.iNj;=(m.Qi.D2.y2.m.si.iw.y.i.iM.N2.
U?..Dl.DS..Sl.lXi.O4.I)7.yS.lW..S4lUS|-..HSUI1.SYMM.SUI'HR=4I)I'RINTJS/ETWISSSTOP
50 100 150
DISTANCE [m]
3.000 a- .986E-03
-6 e- .828E-08
200
— 10,,
29.279 f - -36.16
v = 13.2001
f - -31.64
TUTU:, "PEP. 100 DF.G. FINAL CONFKi . AlKillST! DATA FROM ACD NOTl: 34! DRIFTSDRIFT.DI. l.=6.3?12299DRIFT.D2. l.=3.IOO142ODRIFT.DSEP. 1-2.32X9122DRIFT.DRF, U2.97069WDRIIT.IM. UI3.MIS09WDRIFT.IM. L=2.442SI931*111.1)1.1.I)KIFT.DL2.IWIFT.DL3. U>O.SM(MI971JRI1T.DL4, Ln0.2(W997DRIIT.DCI. UO.54M34UDRIFT.IX'IA. L=O.2733I<M>ORIKT.DC2. L=O.7.W«2IVDRIFT.DC2A. Ufl.73J63.19DRIIT.DC3. L=O.76O«2I9DRIFT.DC4, L=0.2236341DRIFT.DC4A. L=0.2255196DRIIT.DS1. UO.94OH2I8DRIFT.OSH. U2.5I082I8DRIFT.DR06. 1^0.1105DRIFT.DR07. L=O.22O0DRIFT.DRIO. UO.1I38DRIFT.DR1I. U0.I930DRIFT.DR20. L=O.IO58DRIFT.DR2I. L=O.4O5ODR1FT.DR22. L=O.IO«6DR1FTJJR23. L=0.1K50DR1FT.DR24. L-0.113SDRfFT,DR25. L=O.I950DRIFT.DR26. L=O.6O58DR1FT.DR27. UO.0850DRIFT.DSS. L=O.l1 QUADS
l.= l.MK77tl. KQUAl),Q2ll. I.-O.77IOKK. K1=O.(MI2K25.1
I.--I) 'I*)H, Kl=l).OHOIOfi2'J
L-M.WX.l.Vi. KI=-O.22'>.1S4S
I.=0.7.1273:. K M ) 2UO.Wi.Vift. K I =0.27X71304
l.=0..SSX.1.Vi, K 1-0 .24 I42X').14SQUAD.QSI. U0.S5X.1Sft. KI-O.IX2W2775! BF.NniNCi MAGNETSsni-:Nl>.HB. l. = S.4.ANtj|.li.SIIhND.Ill.l. I.=2 0, ANCil.F.-(l.(KKW,l;i-(UKKH,l:.2=(l.(KKM! SEXTHIf)I.E.SSILXT.SI1, 1.-0 2VK2--O.0SEXT.SDI. L=0.2S,K2=<)0
SI-XT.SD. L=O2S.K2=SEXT.SF. I.=(I.25.K2=3.2()WW.SliXT.SIXS. l.=O.25,K2=-(l.«ll S24SEXT^Fft. L=O.25.K2=4 (ISEXT.SI*. L=I).25.K2=-.10X142SEXT.SD7. I.=(I.25.K2=-4OSEXT.SFV. L=O.2S.K2=«I.{1'BEAMI.INF.S
I.INF..SUPF.R=(W)1)1-C.-DOI>EC)I.INE.IOTUEC=(INSERL.CaLL2.CEI.L3.CEUJ.CF.l.l.S.SYMS)LINi;.INSERI.=(INSER.MATCHI.MATCH2.MATC».i.CEIXI)LINE.INSER=(Dl,2'QIH.D2.2<Q2H.DSEP.DJ.9*DRF.D4.Q3)LINE.MATCHI'=(DLI.BLF.DL2.QF1.DRO6.SFI.DRO7,BLF.UW)LlNE.MATCH2>(BB.DC2.0OI.DRin,nsS.SDI.DSS.DRII.BB.&
IX-4A.QF2.1X: I A)LINF..MATCM3=(BB.rx^!.ODI.I)R2()..SO2.l)«2I.HII.IX"4.QF3ll.lNt,CF.U.l=(l)R22.SF.t)R2VBB.rK-2.QI)l.l>K2l».SI).*
87
DR2I.BB,DC4,QFH)LINL,CELL2=<QFH,DR22.SF.DR23.BB,DC2.QD,DR2O.&
SD,DR21,BB,DC4,QFH)LINE,C01X3=<QFH.DR22,SF,DR23,BB.DC2.QD,DR24,4
DSS.SD5,DSS.DR25.BB,DC4,QFH)LINE.CELL4=(QFH.DR22,SF6.DK23,BB,DC2,QD,DR24.&
DSS.SD6,DSS,DR25.BB.DC4.QFH)LINE.CELL5=(QFH.DR22.SF.DR23.BB.DC2,Ql>.DR24.&
DSS,SD7,DSS.DR25,BB,DC4,QFH)L1NE.SYMS=(QFH,DR22.SF,DR23.BB,DC2A.QS2,DR22.*
SD,DR23,BB,DR26,SF9, AUR27.QS1.DSH)
USE.PF.PPRINT.#S/ETWISSSTOP
Addresses
Advanced Lighl SourceLawrence Bcikeley LaboratoryUniversity of CaliforniaBerkeley. California 94720 USA
AI'SArgonne National Lahncalory9700 South Caw AvenueArgnnnc. Illinois «M.W USA
BESSYUmwiillcc 100p. won Berlin wWest GermanyFAX: 82004 I OS
CHESSWilson Synchrotron LabCornell UniversityIthaca, New York 14854 USA
IliSORHiroshima UniversityHigashiscnda d mHiroshimashi. Hiroshima 71(1Japan
HESVRLUniv. of Set. & Tech. of CliiniiHefci. AnhuiPeople's Republic of China
IN™Laboralori Na/iouali ili riascati(KXM4 Prascali. KinnaItaly
Institute of High Energy PhysicsAcademia SinicaBeijingPeople's Republic of China
ESRFB.P. 2203804.1 Grenoble CcdcxFranceFAX: 76 88 2020
HASYLABDESYNotkestrasse 852000 Hamburg 52TEL: (0401 8998 • 0FAX: (040) 8998-3282TELEX: 2 15 124 desy d
Insiuute for Solid Stale PhysicsSynchrotron Radiation LaboratoivUniversity of TokyoMidon-chn, Tanashi. Tokyo IKKJapan
LNLSCaixa Postal 6192 Ccp 1.1081Campinas SP Brazil
LURE91405 Oi sayFrance
M.ix LaboratoryInstitute of PhysicsSnlvcgatan 14223 f>2 LundSweden
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NSLSBuilding 725Drookhaven National LaboratoryUpton, New York 11973 USATEL: 516 282-5257FAX: 516 282-4745TELEX: 6852516 BNL DOE
Pohang l.igl SourcePohang Inst. Sci. & Tech.San 31. Hyoja-dongPohang, Kyungsangbuk-doSouih Korea
RIKENInstitute of Physicsand Chemical ResearchHirosawa 2-1. V/ako-shiSaitanu. 351-01Japan
SERC Daresbury Laboratory
Darushury. Wamngion WA4 4AI)England
Siucotrnnc Triestec/1 Area di RiccrcaPadnciami W34012 TriesteItaly
SSRLP.O. Box 4349Sl.AC Bin 69Slanroril, Cililimua 94305 USA
SURFNational Bureau of StandardsNational Measurement [.inoraloryCmilhcrshiirg, MD 20SW USA
.Synchrotron RidiMkin CenterUniversity of Wisconsin-Madison3725 Schneider DriveSloughton. Wisconsin 53589 USA
TERASElectrotechnical Uiboralory1-1-4 Umczono, Tsukuba-shiIbaraki 305JapanTELEX: 3652570 AISTJ
UVSOR FacilityInstitute for Molecular ScienceMyodaigi. Okazaki 444Japan
Krfcrtims'11K* following hsl IK not intended to give credit to the origi-
nal authors oil a particular subject hut instead Ki indicate thematrnnls used hy the author locninpilc this dalabook.Dul M. Hassclti, LGP Note S04, (I9R4).liol 1 )1 . Book. NKL I'lasnu Formulary, 1987 Revised.Hrl K.L. Hrown * R.V. Scrvranckx. Nuc. Insi. Mcth. A258.
p. 480(1987).Br2 H. Bruck. "Accclcratcucs Circulaircs dc Paniciilcs", Press
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88-2 (1987).H.iI K. Halbach. J. dc Physique. Collnquc Cl, p. CI-211.
(1983).Ilc I KM. Helm, M.J. Lcc, P.I.. Munon & M. Sands, IEEE
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Ed., (1975).Kal Y. Kamiya & M. Kihara, KEK 8316. (1983).Ka2 M. Katoh and Y. Kamiya, l»roc. IEEE PAC, p. 437.
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3(I9S7).
Max LaboraloryInstitute of PhysicsSolvcgatan 1422 < 62 LundSweden
KI-.K
Pholon Factory
1 1 Oho-machi. Tsukiiba-guu
Ibaniki-kcn
305 JapanTEL. (1298 64 1171
TELEX '652 534
Dareshurv Wamnplon WA4 4A1)England
Smcouone Tneslc
c, ) Area dl Ricerca
Padnajim W
'•1(112 Tru-Nt.-
Italy
SSRLP.O. Box 434M
SLAC Bin t-M
Slanfoid. C'aliiinnia 'M3O5 USA
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Pohang Ljght SourcePohang Insl. Sci. & TechSan 31. Hyoja-dongI'ohang, Kyungsangbuk-dnSmith Korea
R1KENInstitute of Physicsand Chemical ResearchHirosawa 2-1. Wako-shiSaitania. 351 01Japan
SERC Darcsbury Laboratory
SURI-National Bureau of StandardsN-atinnal Measurement ljb()raliH\CiauhcrslMirg. MD 2(ISW USA
Synchrotron Rjdiauon CenterUnivi-iMly of Wiscdnsiii-Madison3725 Schneider DnveSlmighton. Wisconsin 5358') USA
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