wl/ibb/e - unt digital library/67531/metadc... · process [6] and the transient collisional...

30
, * /WL/ibb/e.Ha2ba SIMULATION OF THE FUNDAMENTAL AND NONLINEAR HARMOyC OUTPUT FROM AN FEL AMPLIFIER WITH A SOFT X-RAY SEED L S. G. Biedron~, H. P. FreundTT, Y. Li, and S.V. Milton 4&6‘e~~ Advanced Photon Source, Argonne National Laboratory, Argonne Illinois 60439 e ~8JJ$@4 ~ , “h Abstract A single-pass, high-gain free-electron laser (FEL) x-ray amplifier was simulated using the 3D, polychromatic simulation code MEDUSA. The seed for the system is a table-top, soft x-ray laser. The simulated fundamental and nonlinear harmonic x-ray output wavelengths are discussed. 1 INTRODUCTION In a high-gain, single-pass free-electron laser (FEL) amplifier, the input seed laser determines the output wavelength. Nonlinear harmonic interactions in free- electron lasers have been previously discussed in the literature [1-4]. Previous amplifier systems have been limited in reaching soft x-ray wavelengths due to the available seed laser wavelengths. More recently, the advent of table-top, soft x-ray lasers [5] have opened the possibility of using this seed in a master oscillator power amplifier (MOPA) arrangement. Combined with the nonlinear harmonics, significantly shorter longitudinally coherent wavelengths can be achieved. In this paper, the 3D, polychromatic FEL simulation code MEDUSA [3,4] will be used to examine a soft x-ray, table-top laser as the seed in an amplifier FEL. In addition, the resulting nonlinear harmonic power in the system will be discussed. 2 REVIEW OF THEORY 2.1High-Gain, Single-Pass Free-Electron Lasers In a seeded high-gain, single-pass FEL, the seed laser is injected into an undulator in synchronization with a high- quality electron beam (low emittance and energy spread, high peak current, mostly uniform in the transverse and longitudinal planes). As the name suggests, the input seed laser is amplified by the coupling between the radiation and the transverse electron motion. The gain of the system * Work supported by the U.S. Department of Energy, Office of Basic Energy Sciences, under Contract No. W- 31-109-ENG-38. t Argonne and MAX-Lab, University of Lund, Lund S- ~21 00 Sweden H Pemment address, SAIC, McLean VA 22102 depends upon the quality of the beams and undulator” well as the relative arrival time of the electron and laser beams. The ID resonance condition for this FEL interaction is k ~ =XU(1+K2 /2)/2y2, where &is the seed laser and output radiation wavelength, k” is the undulator period, ‘y is the relativistic factor for the electron beam, and K is the undulator parameter K = 0.9377Buku [T-cm], for the magnetic field Bu . A seed laser is not necessary to create a high-gain, single-pass FEL, as the spontaneous radiation shot noise will also couple to the electron beam and begin microbunching. Saturation will be achieved if sut%cient undulator periods are traversed. This phenomenon is known as self-amplified spontaneous emission (SASE). As SASE starts up from noise, the output is also noisy. In a MOPA arrangement, however, the output is more stable and can be fully longitudinally coherent. 2.2 Table-Top, Soft X-ray Lasers Recently, the developments in table-top, soft x-ray lasers have proved a possible seed source for MOPA systems [5]. These table-top x-ray lasers use a variety of high temperature plasma media, with lasing wavelengths from 12 to 60 nm. One of the more versatile methods of generating such table-top x-ray lasers involves the combined use of a chirped pulse amplification (CPA) process [6] and the transient collisional excitation (TCE) scheme [7]. In TCE, a long, low-intensity laser pulse is used to generate a plasma on a target. Next, this plasma is heated briefly by an ultra-short, high-intensity laser pulse. Such heating causes a population inversion in neon- or nickel-like ions. Saturated laser output at a table-top scale from 33 nm down to 12 am has been achieved with these systems [8,9]. 2.3Nonlinear Harmonic Generation Harmonics of the fundamental are present in FELs. As saturation is approached, the bunching occurring at the fundamental due to the interaction of the radiation and electrons causes nonlinear growth of higher harmonics [l- 4]. Due to the natural motion of the electron beam in a planar undulator system, however, odd harmonics are preferentially generated in the forward direction. The gain lengths of the harmonics vary in inverse proportion to the harmonic number. They also allow multiple-wavelength Iasing in FEL systems employing planar undulator systems. The s.brnitted manuscript has been created by the University of Chicago m Operator of Argonne NJtional Laboratory (“Argonne”) under Conuact No, W-31-109-ENG-38 with the U.S. Department of Energy. The U ,S, Government retains for itself, and others acting on its behalf, a paid-up, nonexclusive, irrevocable worldwide license in said iulicle [o reproduce, prepare derivative works, distribute copies to the public, and perform publicly and display publicly, by or on behalf of the Government.

Upload: others

Post on 27-Sep-2020

1 views

Category:

Documents


0 download

TRANSCRIPT

Page 1: WL/ibb/e - UNT Digital Library/67531/metadc... · process [6] and the transient collisional excitation (TCE) scheme [7]. In TCE, a long, low-intensity laser pulse is used to generate

,* /WL/ibb/e.Ha2ba

SIMULATION OF THE FUNDAMENTAL AND NONLINEAR HARMOyCOUTPUT FROM AN FEL AMPLIFIER WITH A SOFT X-RAY SEED L

S. G. Biedron~, H. P. FreundTT, Y. Li, and S.V. Milton 4&6‘e~~Advanced Photon Source, Argonne National Laboratory, Argonne Illinois 60439 e~8JJ$@4 ~

,“h

Abstract

A single-pass, high-gain free-electron laser (FEL) x-rayamplifier was simulated using the 3D, polychromaticsimulation code MEDUSA. The seed for the system is atable-top, soft x-ray laser. The simulated fundamental andnonlinear harmonic x-ray output wavelengths arediscussed.

1 INTRODUCTION

In a high-gain, single-pass free-electron laser (FEL)amplifier, the input seed laser determines the outputwavelength. Nonlinear harmonic interactions in free-electron lasers have been previously discussed in theliterature [1-4]. Previous amplifier systems have beenlimited in reaching soft x-ray wavelengths due to theavailable seed laser wavelengths. More recently, theadvent of table-top, soft x-ray lasers [5] have opened thepossibility of using this seed in a master oscillator poweramplifier (MOPA) arrangement. Combined with thenonlinear harmonics, significantly shorter longitudinallycoherent wavelengths can be achieved. In this paper, the3D, polychromatic FEL simulation code MEDUSA [3,4]will be used to examine a soft x-ray, table-top laser as theseed in an amplifier FEL. In addition, the resultingnonlinear harmonic power in the system will be discussed.

2 REVIEW OF THEORY

2.1High-Gain, Single-Pass Free-ElectronLasers

In a seeded high-gain, single-pass FEL, the seed laser isinjected into an undulator in synchronization with a high-quality electron beam (low emittance and energy spread,high peak current, mostly uniform in the transverse andlongitudinal planes). As the name suggests, the input seedlaser is amplified by the coupling between the radiationand the transverse electron motion. The gain of the system

* Work supported by the U.S. Department of Energy,Office of Basic Energy Sciences, under Contract No. W-31-109-ENG-38.t Argonne and MAX-Lab, University of Lund, Lund S-~21 00 Sweden

H Pemment address, SAIC, McLean VA 22102

depends upon the quality of the beams and undulator”well as the relative arrival time of the electron and laserbeams. The ID resonance condition for this FELinteraction is k ~ =XU(1+K2 /2)/2y2, where &is theseed laser and output radiation wavelength, k” is theundulator period, ‘y is the relativistic factor for theelectron beam, and K is the undulator parameterK = 0.9377Buku [T-cm], for the magnetic field Bu .

A seed laser is not necessary to create a high-gain,single-pass FEL, as the spontaneous radiation shot noisewill also couple to the electron beam and beginmicrobunching. Saturation will be achieved if sut%cientundulator periods are traversed. This phenomenon isknown as self-amplified spontaneous emission (SASE).As SASE starts up from noise, the output is also noisy. Ina MOPA arrangement, however, the output is more stableand can be fully longitudinally coherent.

2.2 Table-Top, Soft X-ray Lasers

Recently, the developments in table-top, soft x-raylasers have proved a possible seed source for MOPAsystems [5]. These table-top x-ray lasers use a variety ofhigh temperature plasma media, with lasing wavelengthsfrom 12 to 60 nm. One of the more versatile methods ofgenerating such table-top x-ray lasers involves thecombined use of a chirped pulse amplification (CPA)process [6] and the transient collisional excitation (TCE)scheme [7]. In TCE, a long, low-intensity laser pulse isused to generate a plasma on a target. Next, this plasma isheated briefly by an ultra-short, high-intensity laser pulse.Such heating causes a population inversion in neon- ornickel-like ions. Saturated laser output at a table-top scalefrom 33 nm down to 12 am has been achieved with thesesystems [8,9].

2.3Nonlinear Harmonic Generation

Harmonics of the fundamental are present in FELs. Assaturation is approached, the bunching occurring at thefundamental due to the interaction of the radiation andelectrons causes nonlinear growth of higher harmonics [l-4]. Due to the natural motion of the electron beam in aplanar undulator system, however, odd harmonics arepreferentially generated in the forward direction. The gainlengths of the harmonics vary in inverse proportion to theharmonic number. They also allow multiple-wavelengthIasing in FEL systems employing planar undulatorsystems.

The s.brnitted manuscript has been created by the University of Chicago m Operator of Argonne NJtional Laboratory (“Argonne”) under Conuact No, W-31-109-ENG-38with the U.S. Department of Energy. The U ,S, Government retains for itself, and others acting on its behalf, a paid-up, nonexclusive, irrevocable worldwide license in saidiulicle [o reproduce, prepare derivative works, distribute copies to the public, and perform publicly and display publicly, by or on behalf of the Government.

Page 2: WL/ibb/e - UNT Digital Library/67531/metadc... · process [6] and the transient collisional excitation (TCE) scheme [7]. In TCE, a long, low-intensity laser pulse is used to generate

DISCLAIMER

This report was,.prepared as an account of work sponsoredby an agency of the United States Government. Neitherthe United States Government nor any agency thereof, norany of their employees, make any warranty, express orimplied, or assumes any legal liability or responsibility forthe accuracy, completeness, or usefulness of anyinformation, apparatus, product, or process disclosed, orrepresents that its use would not infringe privately ownedrights. Reference herein to any specific commercialproduct, process, or service by trade name, trademark,manufacturer, or otherwise does not necessarily constituteor imply its endorsement, recommendation, or favoring bythe United States Government or any agency thereof. Theviews and opinions of authors expressed herein do notnecessarily state or reflect those of the United StatesGovernment or any agency thereof.

Page 3: WL/ibb/e - UNT Digital Library/67531/metadc... · process [6] and the transient collisional excitation (TCE) scheme [7]. In TCE, a long, low-intensity laser pulse is used to generate

DISCLAIMER

Portions of this document may be illegiblein electronic image products. Images areproduced from the best available originaldocument.

Page 4: WL/ibb/e - UNT Digital Library/67531/metadc... · process [6] and the transient collisional excitation (TCE) scheme [7]. In TCE, a long, low-intensity laser pulse is used to generate

.

.

THE EVOLUTION OF ANL CMT GLOVEBOXES

INTRODUCTION

‘ Argonne National Laboratory

● Chemical Technology Division (CMT)

● Modular Gloveboxes Designed forExperimental Work

– Laboratory Scale

– Engineering Scale

● Experimental Work Includes Equipmentand Process Development for:

Pyrochemical

Nuclear Waste Treatment

Electrochemistry

#o?4<‘4

.4)!)RFMAGs2000_l

( Q ] Argonne National Laboratory%‘2. $’%*%@**” .

Page 5: WL/ibb/e - UNT Digital Library/67531/metadc... · process [6] and the transient collisional excitation (TCE) scheme [7]. In TCE, a long, low-intensity laser pulse is used to generate

.

THE EVOLUTION OF ANL CMT GLOVEBOXES

HISTORY

● The First ANL-CMT Division ModularGlovebox was Designed and Installedin 1959. It was designated as theCENHAM glovebox.

● Desian Obiective:

w ●

Provide Modular Configuration

Provide Controlled AtmosphereEnvironment

Maximize Viewing Accessibility

Provide “Standardized” Work Area forLaboratory Research Work

Provide Modular Utility Service Access

Include User-Friendly Considerations

#OwL

A%* RFMAGs2000_2

“~’ o ~ Argonne National Laboratory..% &*-2.*4

G .

%7 0$@

Page 6: WL/ibb/e - UNT Digital Library/67531/metadc... · process [6] and the transient collisional excitation (TCE) scheme [7]. In TCE, a long, low-intensity laser pulse is used to generate

THE EVOLUTION OF ANL CMT GLOVEBOXES

GLOVEBOX DESIGN REQUIRESAWARENESS OF USER NEEDS

Q Evolution of Design Over the Past 40Years

“ Request for New Gloveboxes UsuallyBased Upon Similar Attributes of anExisting Enclosure Plus ParticularProject Changes for Use.

● Discussion with Staff and LaboratoryOperating Personnel.

● Considerations:

– Simplicity in Design

– Cost Saving

– Schedule

● Defining “What is Necessary” and“What Would be Nice.”

RFMAGS2000_3

National Laboratory

Page 7: WL/ibb/e - UNT Digital Library/67531/metadc... · process [6] and the transient collisional excitation (TCE) scheme [7]. In TCE, a long, low-intensity laser pulse is used to generate

.

THE EVOLUTION OF ANL CMT GLOVEBOXES

USER-FRIENDLY GLOVEBOX DESIGN

● Gloveboxes Use a Modular DesignConcept

“ Glovebox Size is Designated asModules in Length and Tiers in Height

‘ Basic Module is 42 inch Cube

c Modular End Plates Provide for:

– Utility Services

– Ventilation/Purification

– Filter Housings

– Transfer Locks

– Bagpotts

System

Page 8: WL/ibb/e - UNT Digital Library/67531/metadc... · process [6] and the transient collisional excitation (TCE) scheme [7]. In TCE, a long, low-intensity laser pulse is used to generate

THE EVOLUTION OF ANL CMT GLOVEBOXES

MATERIALS OF CONSTRUCTION

● Steel Shell (Painted)

Q Stainless Steel Shell

“ Steel Support Frame

● Gloveports

c Glass Windows

Page 9: WL/ibb/e - UNT Digital Library/67531/metadc... · process [6] and the transient collisional excitation (TCE) scheme [7]. In TCE, a long, low-intensity laser pulse is used to generate

THE EVOLUTION OF ANL CMT GLOVEBOXES

STRUCTURE

Glovebox

Structural

Unistrut

Floor

She

Elements

End Plates

Hoists

Floor Wells

RFMAGS2000_6

Page 10: WL/ibb/e - UNT Digital Library/67531/metadc... · process [6] and the transient collisional excitation (TCE) scheme [7]. In TCE, a long, low-intensity laser pulse is used to generate

.

THE EVOLUTION OF ANL CMT GLOVEBOXES

UTILITIES

● Process Feedthroughs for Services

– Electrical

– Instrument

– Gas or Liquid

● Lighting

Argonne National

RFMAGS2000_7

Laboratory

Page 11: WL/ibb/e - UNT Digital Library/67531/metadc... · process [6] and the transient collisional excitation (TCE) scheme [7]. In TCE, a long, low-intensity laser pulse is used to generate

THE EVOLUTION OF ANL CMT GLOVEBOXES

TRANSFER SYSTEMS

Bagout

Large

Small

Horizontal

Horizontal

Vertical Transfer

S~hincter

Transfer

Transfer

Lock

Lock.’

Lock

RFMAGS2000_8

Page 12: WL/ibb/e - UNT Digital Library/67531/metadc... · process [6] and the transient collisional excitation (TCE) scheme [7]. In TCE, a long, low-intensity laser pulse is used to generate

THE EVOLUTION OF ANL CMT GLOVEBOXES

QA APPLICATION

Management Control

– Team Approach

– Process Development

– Design and Fabrication

– Scheduling

Design Review

Design for Manufacturability Reviews(DFM)

System Design Description

Safety Review

Operational Readiness Review

#lw.4c

.(!8!)* %% RFMAGS2000_9

3*

[0 ? Argonne National Laboratory*#%!%*Y~,s

Page 13: WL/ibb/e - UNT Digital Library/67531/metadc... · process [6] and the transient collisional excitation (TCE) scheme [7]. In TCE, a long, low-intensity laser pulse is used to generate

.

THE EVOLUTION OF ANL CMT GLOVEBOXES

WINDOWS

Q Window Viewing Area ComprisesApproximately 60% of the GloveboxSide Walls that Suffices for MonitoringExperimental Equipment and ProcessOperation

“ Weatherstrip Type “Zipper” Seal Usedfor Window Installation

Q Window Concept

Nominal 36 Inch Square Windows andWindow Openings with Rounded Corners

3/8 Inch Thick Laminated Safety GlassWindows

Glovepon% are Attached Through theWindows

@10N4c

A+ RFMAGs2000_l o*+* %+

;.< ) Argonne National Laboratory“%%” &%eyOF0+’

Page 14: WL/ibb/e - UNT Digital Library/67531/metadc... · process [6] and the transient collisional excitation (TCE) scheme [7]. In TCE, a long, low-intensity laser pulse is used to generate

>

THE EVOLUTION OF ANL CMT GLOVEBOXES

I

i-.I

Hoist and well

fi3[[0 o“ a

7!

v

\

-standard

IHoist ●

/“-we”

+T *N4 I-

Af4 RFMAGs2000_l 1

? 0 ‘! Argonne National Laboratoryc%-ii%?y*?,68@ .

Page 15: WL/ibb/e - UNT Digital Library/67531/metadc... · process [6] and the transient collisional excitation (TCE) scheme [7]. In TCE, a long, low-intensity laser pulse is used to generate

THE EVOLUTION OF ANL CMT GLOVEBOXES

Glovebox Baseboard Duct

.

,— Electrical

QOutlet

‘GasDistribution

InsideDuct Covet- ~lovebox !nstrumenFloor Outlek

tation

Page 16: WL/ibb/e - UNT Digital Library/67531/metadc... · process [6] and the transient collisional excitation (TCE) scheme [7]. In TCE, a long, low-intensity laser pulse is used to generate

THE EVOLUTION OF ANL CMT GLOVEBOXES

GLOVEBOX SUPPORT STAND ‘

F- —+\

*+TioNAt

A# %e,e RFMAGs2000_l 3

# .+.8<. ) Argonne National Laboratory. %%%..rQF~+”-t

Page 17: WL/ibb/e - UNT Digital Library/67531/metadc... · process [6] and the transient collisional excitation (TCE) scheme [7]. In TCE, a long, low-intensity laser pulse is used to generate

4 MODULE -1 1/2 TIER GLOVEBOX

1

THE EVOLUTION OF ANL CMT GLOVEBOXES

*ATFJW

“Ah RFMAGs2000_l 4

( 0 ~ Argonne National Laboratory$*%%%orG+’+’ .

Page 18: WL/ibb/e - UNT Digital Library/67531/metadc... · process [6] and the transient collisional excitation (TCE) scheme [7]. In TCE, a long, low-intensity laser pulse is used to generate

THE EVOLUTION OF ANL CMT GLOVEBOXES

CiLOVEBOX2 MODULE -2 TIER

U.

#m4.4’

+

A*, %+ RFMAGS2000_15

[“”;.0 Argonne National Laboratory%’ g*“%*,~~fl

Page 19: WL/ibb/e - UNT Digital Library/67531/metadc... · process [6] and the transient collisional excitation (TCE) scheme [7]. In TCE, a long, low-intensity laser pulse is used to generate

.

THE EVOLUTION OF ANL CMT GLOVEBOXES

GAS RECIRCULATION SYSTEM ‘-

EMERGENCYIIINLETC3REXHAUST

BUBBLER

/

,TION

Page 20: WL/ibb/e - UNT Digital Library/67531/metadc... · process [6] and the transient collisional excitation (TCE) scheme [7]. In TCE, a long, low-intensity laser pulse is used to generate

THE EVOLUTION OF ANL CMT GLOVEBOXES

GLOVEBOX ASSEMBLY .

LJ ‘d!)’.

.

Page 21: WL/ibb/e - UNT Digital Library/67531/metadc... · process [6] and the transient collisional excitation (TCE) scheme [7]. In TCE, a long, low-intensity laser pulse is used to generate

r

THE EVOLUTION OF ANL CMT GLOVEBOXES

GLOVEBOX FILTER ACCESSIBILITY

F1

@ou4<

A#%* RFMAGS2000_l 8

$“<. ! Argonne National Laboratory%“b #%**V~FG*’$ .

Page 22: WL/ibb/e - UNT Digital Library/67531/metadc... · process [6] and the transient collisional excitation (TCE) scheme [7]. In TCE, a long, low-intensity laser pulse is used to generate

THE EVOLUTION OF ANL CMT GLOVEBOXES

EPOXY RESIN

Inside Weld Joints are Caulked with anEpoxy Resin.

The Epoxy Resin (ABAWELD) has beenUsed on Gloveboxes in CMT for ManyYears

The Caulked Joints Provide a SmoothCorner Fillet Designed for Easy Clean-Up

.

Page 23: WL/ibb/e - UNT Digital Library/67531/metadc... · process [6] and the transient collisional excitation (TCE) scheme [7]. In TCE, a long, low-intensity laser pulse is used to generate

.

THE EVOLUTION OF ANL CMT GLOVEBOXES

WEATHERSTRIP INSTALLATION

GUN NOZZLE

SEALINGCOMPOUND

WEATHERSTRIP

,

GLASS WINDOW

GLOVEBOXWALL

.“

Argonne National Laboratory

RFMAGs2000_20

Page 24: WL/ibb/e - UNT Digital Library/67531/metadc... · process [6] and the transient collisional excitation (TCE) scheme [7]. In TCE, a long, low-intensity laser pulse is used to generate

.

THE EVOLUTION OF ANL CMT GLOVEBOXES

GLASS TYPE

● Glass laminate per ASTM Cl 172-91

● Two Iite laminate ofq3 quality glass

● Each Iite is .19 inch

Kind LA, Class 1,

thick with overacomposite thickness of .38 inch

@ WJ4 e

A

*,+&* RFMAGs2000_21

(‘ () ~ Argonne National Laboratory-2.%e J@@*F6*~

Page 25: WL/ibb/e - UNT Digital Library/67531/metadc... · process [6] and the transient collisional excitation (TCE) scheme [7]. In TCE, a long, low-intensity laser pulse is used to generate

,

THE EVOLUTION OF ANL CMT GLOVEBOXES

FAILURE OF GLOVEBOX WINDOWWITH GLOVEPORTS

c

E

Page 26: WL/ibb/e - UNT Digital Library/67531/metadc... · process [6] and the transient collisional excitation (TCE) scheme [7]. In TCE, a long, low-intensity laser pulse is used to generate

c

E

FAILURE OF GLOVEBOX WINDOWWITHOUT GLOVEPORTS

,

.

THE EVOLUTION OF ANL CMT GLOVEBOXES

Page 27: WL/ibb/e - UNT Digital Library/67531/metadc... · process [6] and the transient collisional excitation (TCE) scheme [7]. In TCE, a long, low-intensity laser pulse is used to generate

.

THE EVOLUTION OF ANL CMT GLOVEBOXES

WINDOW TEST RESULTS

● Window with four gloveports

Test terminated due to structural failure ofthe window glass

Cracks developed in the glass extendingacross the two lower gloveports

Test pressure at failure was 17 inches ofwater

No evidence of seal failure

@ ‘~’ %..

ARFMAGS2000_24

(’ 6 ~ Argonne National Laboratory% ~0*

I..

+, *6 6*$

Page 28: WL/ibb/e - UNT Digital Library/67531/metadc... · process [6] and the transient collisional excitation (TCE) scheme [7]. In TCE, a long, low-intensity laser pulse is used to generate

,

THE EVOLUTION OF ANL CMT GLOVEBOXES

WINDOW TEST RESULTS -

● Window without gloveports

– Test terminated due to structural failure ofthe window glass

– Crack developedfrom the center

in the glass radiating out

– Test pressure at failure was 30 inches ofwater (> 2 psig)

– No evidence of seal failure

RFMAGS2000_25

me National Laboratory.

Page 29: WL/ibb/e - UNT Digital Library/67531/metadc... · process [6] and the transient collisional excitation (TCE) scheme [7]. In TCE, a long, low-intensity laser pulse is used to generate

THE EVOLUTION OF ANL CMT GLOVEBOXES

INTERIOR ENVIRONMENTATMOSPHERE

● Flow Controls - Once Through Gas

Gas Recirculation System -● InertRequiresFilters

● Pressure

Purification System with

Controls

Page 30: WL/ibb/e - UNT Digital Library/67531/metadc... · process [6] and the transient collisional excitation (TCE) scheme [7]. In TCE, a long, low-intensity laser pulse is used to generate

THE EVOLUTION OF ANL CMT GLOVEBOXES

SUMMARY

Design Approach BasedFriendly Concept

Upon User-

Utilization of ExistingDesigns

Cost Effective

Schedule

Component

Adaptable to Project Process ChangesWithout Losing Overall Effectivenessof “User-Friendly” Approach.

RFMAGS2000_27

>