304L 6.35*1mm Abahlinzeki bamashubhu ensimbi engagqwali ahlanganiswe ,Ukuboniswa kwenduku ye-lithium enamandla yokukhiqiza ama-neutron aqondile

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STAINLESS STEEL COIL TUBE INDLELA YOKUCACISA

304L 6.35*1mm Abahlinzeki bamashubhu ensimbi engenasici

Okujwayelekile I-ASTM A213 (I-Average Wall) ne-ASTM A269
I-Stainless Steel Coil Tubing Ngaphandle Kobubanzi 1/16” ukuya ku-3/4″
Ishubhu ye-Stainless Steel Coil .010″ Ukudlula .083”
I-Stainless Steel Coil Tubes Amabanga SS 201, SS 202, SS 304, SS 304L, SS 309, SS 310, SS 316, SS 316L, SS 317L, SS 321, SS 347, SS 904L
Usayizi Rnage 5/16, 3/4, 3/8, 1-1/2, 1/8, 5/8, 1/4, 7/8, 1/2, 1, 3/16 amayintshi
Ukuqina I-Micro kanye ne-Rockwell
Ukubekezelelana I-D4/T4
Amandla I-Burst and Tensile

STAINLESS STEEL COIL TUBING AMABANGA ALINGANAYO

IZINGA I-WERKSTOFF NR. I-UNS I-JIS BS I-GOST AFNOR EN
I-SS 304 1.4301 I-S30400 I-SUS 304 304S31 08Х18Н10 I-Z7CN18-09 I-X5CrNi18-10
I-SS 304L 1.4306 / 1.4307 I-S30403 I-SUS 304L 3304S11 03Х18Н11 I-Z3CN18-10 X2CrNi18-9 / X2CrNi19-11
I-SS 310 1.4841 S31000 I-SUS 310 310S24 20Ch25N20S2 - I-X15CrNi25-20
I-SS316 1.4401 / 1.4436 I-S31600 I-SUS 316 316S31 / 316S33 - Z7CND17-11-02 X5CrNiMo17-12-2 / X3CrNiMo17-13-3
I-SS 316L 1.4404 / 1.4435 I-S31603 I-SUS 316L 316S11 / 316S13 03Ch17N14M3 / 03Ch17N14M2 Z3CND17-11-02 / Z3CND18-14-03 X2CrNiMo17-12-2 / X2CrNiMo18-14-3
I-SS 317L 1.4438 I-S31703 I-SUS 317L - - - X2CrNiMo18-15-4
I-SS 321 1.4541 I-S32100 I-SUS 321 - - - I-X6CrNiTi18-10
SS 347 1.4550 S34700 I-SUS 347 - Idatha ye-08Ch18N12B - I-X6CrNiNb18-10
I-SS904L 1.4539 N08904 I-SUS 904L 904S13 I-STS 317J5L Z2 NCDU 25-20 X1NiCrMoCu25-20-5

I-SS COIL TUBE COMPOSIL CHEMICAL

Ibanga C Mn Si P S Cr Mo Ni N Ti Fe
I-SS 304 Coil Tube imiz. 18.0 8.0
ubuningi. 0.08 2.0 0.75 0.045 0.030 20.0 10.5 0.10
I-SS 304L Coil Tube imiz. 18.0 8.0
ubuningi. 0.030 2.0 0.75 0.045 0.030 20.0 12.0 0.10
I-SS 310 Coil Tube 0.015 ubuningi 2 ubuningi 0.015 ubuningi 0.020 ubuningi 0.015 ubuningi 24.00 26.00 0.10 ubuningi 19.00 21.00 54.7 imiz
I-SS 316 Coil Tube imiz. 16.0 2.03.0 10.0
ubuningi. 0.035 2.0 0.75 0.045 0.030 18.0 14.0
I-SS 316L Coil Tube imiz. 16.0 2.03.0 10.0
ubuningi. 0.035 2.0 0.75 0.045 0.030 18.0 14.0
I-SS 317L Coil Tube 0.035 ubuningi 2.0 ubuningi 1.0 ubuningi 0.045 ubuningi 0.030 ubuningi 18.00 20.00 3.00 4.00 11.00 15.00 57.89 imiz
I-SS 321 Coil Tube 0.08 ubuningi 2.0 ubuningi 1.0 ubuningi 0.045 ubuningi 0.030 ubuningi 17.00 19.00 9.00 12.00 0.10 ubuningi 5(C+N) 0.70 ubuningi
I-SS 347 Coil Tube 0.08 ubuningi 2.0 ubuningi 1.0 ubuningi 0.045 ubuningi 0.030 ubuningi 17.00 20.00 9.0013.00
I-SS 904L Coil Tube imiz. 19.0 4.00 23.00 0.10
ubuningi. 0.20 2.00 1.00 0.045 0.035 23.0 5.00 28.00 0.25

STAINLESS STEEL COIL MECHANICAL PROPERTIES

Ibanga Ukuminyana I-Melting Point Amandla Okuqina Amandla Esivuno (0.2%Offset) Ukwelula
I-SS 304/ 304L I-Coil Tubing 8.0 g/cm3 1400 °C (2550 °F) Psi 75000 , MPa 515 Psi 30000 , MPa 205 35 %
I-SS 310 Coil Tubing 7.9 g/cm3 1402 °C (2555 °F) Psi 75000 , MPa 515 Psi 30000 , MPa 205 40 %
I-SS 306 Coil Tubing 8.0 g/cm3 1400 °C (2550 °F) Psi 75000 , MPa 515 Psi 30000 , MPa 205 35 %
I-SS 316L Coil Tubing 8.0 g/cm3 1399 °C (2550 °F) Psi 75000 , MPa 515 Psi 30000 , MPa 205 35 %
I-SS 321 Coil Tubing 8.0 g/cm3 1457 °C (2650 °F) Psi 75000 , MPa 515 Psi 30000 , MPa 205 35 %
I-SS 347 Coil Tubing 8.0 g/cm3 1454 °C (2650 °F) Psi 75000 , MPa 515 Psi 30000 , MPa 205 35 %
I-SS 904L Coil Tubing 7.95 g/cm3 1350 °C (2460 °F) Psi 71000 , MPa 490 I-Psi 32000, i-MPa 220 35 %

Njengenye indlela yocwaningo lwama-reactors enuzi, ijeneretha ye-neutron eqhutshwa yi-accelerator esebenzisa umshayeli we-lithium-ion beam ingase ibe ikhandidethi elithembisayo ngoba ikhiqiza imisebe emincane engadingeki.Kodwa-ke, kwakunzima ukuletha ugongolo oluqinile lwe-lithium ion, futhi ukusetshenziswa okungokoqobo kwamadivayisi anjalo kwakubhekwa njengento engenakwenzeka.Inkinga enzima kakhulu yokugeleza kwe-ion enganele yaxazululwa ngokusebenzisa uhlelo oluqondile lokufakelwa kwe-plasma.Kulolu hlelo, i-high-density pulsed plasma ekhiqizwe i-laser ablation ye-lithium metal foil ijovwa kahle futhi isheshiswe i-high-frequency quadrupole accelerator (RFQ accelerator).Sizuze umthamo omkhulu wamanje we-35 mA osheshiselwe ku-1.43 MeV, okungama-oda amabili obukhulu obungaphezulu kunomjovo ojwayelekile kanye namasistimu e-accelerator angahlinzeka.
Ngokungafani nama-X ray noma izinhlayiya ezishajiwe, ama-neutron anokujula okukhulu kokungena kanye nokusebenzisana okuyingqayizivele nodaba olujiyile, okuwenza abe ama-probe aguquguqukayo kakhulu okutadisha izakhiwo zezinto1,2,3,4,5,6,7.Ikakhulukazi, amasu okuhlakazeka kwe-neutron avame ukusetshenziselwa ukutadisha ukwakheka, ukwakheka, nokucindezeleka kwangaphakathi endabeni efingqiwe futhi anganikeza ulwazi oluningiliziwe mayelana nezinhlanganisela zokulandela umkhondo kuma-alloys ensimbi okunzima ukuwabona kusetshenziswa i-X-ray spectroscopy8.Le ndlela ibhekwa njengethuluzi elinamandla kusayensi eyisisekelo futhi isetshenziswa abakhiqizi bezinsimbi nezinye izinto.Muva nje, i-neutron diffraction isetshenziselwe ukuthola izingcindezi eziyinsalela ezingxenyeni zemishini ezifana nezingxenye zesitimela nezindiza9,10,11,12.Amaneutron nawo asetshenziswa emithonjeni kawoyela negesi ngoba abanjwa kalula ngezinto ezinothile ngeproton13.Izindlela ezifanayo nazo zisetshenziswa kwezobunjiniyela bomphakathi.Ukuhlola i-neutron engacekeli phansi iyithuluzi elisebenzayo lokuthola amaphutha afihliwe ezakhiweni, emhubheni nasemabhulohweni.Ukusetshenziswa kwemishayo ye-neutron kusetshenziswa kakhulu ocwaningweni lwesayensi nasezimbonini, eziningi zazo eziye zathuthukiswa ngokomlando kusetshenziswa ama-reactors enuzi.
Kodwa-ke, ngokuvumelana emhlabeni wonke mayelana nokungasabalala kwezikhali zenuzi, ukwakha ama-reactor amancane ngezinjongo zocwaningo kuya ngokuya kuba nzima.Ngaphezu kwalokho, ingozi yakamuva yaseFukushima yenze ukwakha iziphehlimandla zenuzi kucishe kwamukeleke emphakathini.Ngokuphathelene nalo mkhuba, isidingo semithombo ye-neutron kuma-accelerator siyakhula2.Njengenye indlela yama-reactors enuzi, imithombo eminingana emikhulu ye-neutron ehlukanisa i-accelerator isivele iyasebenza14,15.Kodwa-ke, ukuze kusetshenziswe kahle kakhulu izakhiwo zemishayo ye-neutron, kuyadingeka ukwandisa ukusetshenziswa kwemithombo ehlangene kuma-accelerator, 16 okungenzeka kube yizikhungo zocwaningo zezimboni neyunivesithi.Imithombo ye-accelerator neutron yengeze amandla nemisebenzi emisha ngaphezu kokusebenza njengokumiselela iziphehli ze-nuclear14.Isibonelo, ijeneretha eshayelwa yi-linac ingakha kalula umfudlana wama-neutron ngokushintsha induku yokushayela.Uma esekhishiwe, kunzima ukulawula ama-neutron futhi izilinganiso zemisebe kunzima ukuzihlaziya ngenxa yomsindo odalwa ama-neutron angemuva.I-neutron eshaywayo elawulwa yi-accelerator igwema le nkinga.Kuphakanyiswe amaphrojekthi amaningana asuselwa kubuchwepheshe be-proton accelerator emhlabeni jikelele17,18,19.Ukusabela okuthi 7Li(p, n)7Be kanye no-9Be(p, n)9B kuvame ukusetshenziswa kakhulu kumajeneretha e-neutron ahlangene aqhutshwa yi-proton ngenxa yokuthi ahambisana ne-endothermic20.Imisebe eyeqile kanye nodoti okhipha imisebe kungancishiswa uma amandla akhethelwe ukujabulisa i-proton beam engaphezulu kancane kwevelu yomkhawulo.Kodwa-ke, isisindo se-nucleus eqondiwe sikhulu kakhulu kune-protons, futhi ama-neutron atholakalayo ahlakazeka kuzo zonke izinhlangothi.Ukusondelana okunjalo nokukhishwa kwe-isotropic kwe-neutron flux kuvimbela ukuthuthwa okusebenzayo kwama-neutron entweni yocwaningo.Ngaphezu kwalokho, ukuze uthole umthamo odingekayo we-neutron endaweni yento, kuyadingeka ukwandisa kakhulu kokubili inani lama-proton ahambayo namandla awo.Ngenxa yalokho, imithamo emikhulu yemisebe ye-gamma nama-neutron azosakazeka ngama-engeli amakhulu, acekele phansi inzuzo yokusabela kwe-endothermic.Ijeneretha ye-neutron esekelwe ku-accelerator ejwayelekile inokuvikela emisebeni enamandla futhi iyingxenye enkulu yesistimu.Isidingo sokwandisa amandla okushayela ama-proton ngokuvamile sidinga ukwanda okwengeziwe kosayizi wesikhungo sokusheshisa.
Ukuze kunqotshwe ukushiyeka okuvamile kwemithombo evamile ye-neutron ehlangene kuma-accelerator, uhlelo lokusabela lwe-inversion-kinematic lwahlongozwa21.Kulolu hlelo, i-lithium-ion beam esindayo isetshenziswa njengegayidi yomhlahlandlela esikhundleni se-proton beam, eqondise izinto ezicebile nge-hydrogen ezifana namaplastiki e-hydrocarbon, ama-hydrides, i-hydrogen gas, noma i-hydrogen plasma.Ezinye izindlela ziye zacatshangelwa, njengemishayo eqhutshwa yi-beryllium ion, nokho, i-beryllium iwubuthi obudinga ukunakekelwa okukhethekile ekusingatheni.Ngakho-ke, i-lithium beam iyona efaneleka kakhulu kuma-inversion-kinematic reaction schemes.Njengoba umfutho we-lithium nuclei mkhulu kune-proton, isikhungo sokungqubuzana kwezikhali zenuzi silokhu siqhubekela phambili, futhi ama-neutron nawo akhishwa phambili.Lesi sici siqeda kakhulu imisebe ye-gamma engadingeki kanye nokukhishwa kwe-neutron ye-engeli ephezulu22.Ukuqhathaniswa kwecala elivamile lenjini ye-proton kanye nesimo se-kinematics esiphambene siboniswa kuMfanekiso 1.
Umdwebo wama-engeli okukhiqiza i-neutron we-proton nemishayo ye-lithium (edwetshwe nge-Adobe Illustrator CS5, 15.1.0, https://www.adobe.com/products/illustrator.html).(a) Amaneutron angakhishwa kunoma iyiphi indlela ngenxa yokusabela ngenxa yokuthi ama-proton anyakazayo ashaya ama-athomu asinda kakhulu wethagethi ye-lithium.(b) Ngokuphambene, uma umshayeli we-lithium-ion eqhumisa ithagethi ecebile nge-hydrogen, ama-neutron akhiqizwa kukhoni encane eya phambili ngenxa yesivinini esiphezulu sesikhungo sobuningi besistimu.
Kodwa-ke, ambalwa kuphela amajeneretha e-neutron e-kinematic aphambene akhona ngenxa yobunzima bokukhiqiza ukugeleza okudingekayo kwama-ion asindayo ngokushaja okuphezulu uma kuqhathaniswa nama-proton.Zonke lezi zitshalo zisebenzisa imithombo ye-sputter ion engalungile ngokuhlangana nama-accelerator e-tandem electrostatic.Ezinye izinhlobo zemithombo ye-ion ziye zahlongozwa ukuze kwandiswe ukusebenza kahle kwe-beam acceleration26.Kunoma ikuphi, i-lithium-ion beam current etholakalayo ikhawulelwe ku-100 µA.Kuphakanyiswe ukuthi kusetshenziswe i-1 mA ye-Li3 + 27, kodwa le ndlela ye-ion beam yamanje ayizange iqinisekiswe yile ndlela.Ngokuya kokuqina, ama-accelerator e-lithium beam awakwazi ukuncintisana nama-accelerators we-proton beam lapho i-proton yawo ephezulu yamanje idlula i-10 mA28.
Ukuze usebenzise ijeneretha ye-neutron ehlangene esekelwe kugongolo lwe-lithium-ion, kunenzuzo ukukhiqiza amandla aphezulu angenawo ama-ion.Ama-ion ayasheshisa futhi aqondiswa amandla kazibuthe, futhi izinga eliphezulu lokushaja liholela ekusheshiseni okuphumelelayo.Abashayeli be-Li-ion beam badinga i-Li3+ peak currents ezingaphezu kuka-10 mA.
Kulo msebenzi, sibonisa ukusheshisa kwemishayo ye-Li3+ enamagagasi aphezulu afinyelela ku-35 mA, aqhathaniseka nama-accelerator e-proton athuthukile.Ugongolo lwe-lithium ion lwangempela lwadalwa kusetshenziswa i-laser ablation kanye ne-Direct Plasma Implantation Scheme (DPIS) eyasungulwa ekuqaleni ukusheshisa i-C6+.Irediyo edizayinelwe ngokwezifiso i-quadrupole linac (RFQ linac) yaklanywa kusetshenziswa isakhiwo esinezinduku ezine.Siqinisekise ukuthi i-beam esheshisayo inamandla okubaliwe aphezulu wokuhlanzeka.Uma isigxobo se-Li3 + sibanjwa ngokuphumelelayo futhi sisheshiswe yi-accelerator ye-radio frequency (RF), isigaba esilandelayo se-linac (i-accelerator) sisetshenziselwa ukunikeza amandla adingekayo ukuze kukhiqizwe i-neutron flux eqinile kusukela ekuhlosweni.
Ukusheshiswa kwama-ion okusebenza okuphezulu kuwubuchwepheshe obusungulwe kahle.Umsebenzi osele wokubona ijeneretha entsha ye-neutron ehlangene esebenza kahle kakhulu ukukhiqiza inqwaba yama-ion e-lithium asuswe ngokuphelele futhi kwakhiwe isakhiwo seqoqo esihlanganisa uchungechunge lwama-ion pulses avumelaniswa nomjikelezo we-RF kusisheshisi.Imiphumela yokuhlolwa okuklanyelwe ukufeza lo mgomo ichazwe ezigatshaneni ezintathu ezilandelayo: (1) ukukhiqizwa kwe-lithium-ion beam engenalutho, (2) ukusheshisa kwe-beam kusetshenziswa i-RFQ linac eklanywe ngokukhethekile, kanye (3) nokusheshisa ukuhlaziya. ye-beam ukuhlola okuqukethwe kwayo.E-Brookhaven National Laboratory (BNL), sakhe ukusetha kokuhlola okuboniswe kuMfanekiso 2.
Ukubuka konke kokusetha kokuhlolwa kokuhlaziywa okusheshisiwe kwemishayo ye-lithium (eboniswa yi-Inkscape, 1.0.2, https://inkscape.org/).Ukusuka kwesokudla kuye kwesobunxele, i-laser-ablative plasma ikhiqizwa egumbini lokusebenzisana nethagethi ye-laser futhi ilethwe ku-RFQ linac.Lapho kungena isisheshisi se-RFQ, ama-ion ahlukaniswa ku-plasma futhi ajovwe kusisheshisi se-RFQ ngokusebenzisa inkambu kagesi engazelelwe edalwe umehluko wamandla kagesi angu-52 kV phakathi kwe-electrode yokukhipha kanye ne-electrode ye-RFQ endaweni yokukhukhuleka.Ama-ion akhishiwe asheshiswa ukusuka ku-22 keV/n ukuya ku-204 keV/n kusetshenziswa ama-electrode e-RFQ angamamitha angu-2 ubude.I-transformer yamanje (CT) efakwe ekuphumeni kwe-linac ye-RFQ inikeza ukukala okungabhubhisi kwe-ion beam current.I-beam igxilwe yizibuthe ezintathu ze-quadrupole futhi iqondiswe kumagnet we-dipole, ehlukanisa futhi iqondise ugongolo lwe-Li3 + kumtshina.Ngemuva komkejana, kusetshenziswa ipulasitiki ehoxiswayo ye-scintillator kanye nenkomishi ye-Faraday (FC) enokuchema okungafika ku- -400 V ukuze kutholwe i-beam esheshayo.
Ukuze ukhiqize i-ionized lithium ion ngokugcwele (Li3+), kuyadingeka ukwakha i-plasma enezinga lokushisa elingaphezu kwamandla e-ionization wesithathu (122.4 eV).Sazama ukusebenzisa i-laser ablation ukuze sikhiqize i-plasma enezinga eliphezulu lokushisa.Lolu hlobo lomthombo we-laser ion aluvamile ukusetshenziselwa ukukhiqiza imishayo ye-lithium ion ngoba insimbi ye-lithium iyasebenza futhi idinga ukuphathwa okukhethekile.Senze isistimu yokulayisha eqondiwe ukuze sinciphise umswakama nokungcoliswa komoya lapho sifaka i-lithium foil egumbini lokusebenzisana le-vacuum laser.Konke ukulungiswa kwezinto kwenziwa endaweni elawulwayo ye-argon eyomile.Ngemva kokufakwa kwecwecwe le-lithium ekamelweni eliqondiwe nge-laser, ucwecwe lwakhanyiswa ngemisebe ye-laser ye-pulsed Nd:YAG ngamandla angu-800 mJ ukushaya ngakunye.Lapho kugxilwe kukho, ukuminyana kwamandla e-laser kulinganiselwa ku-1012 W/cm2.I-Plasma yenziwa lapho i-pulsed laser ibhubhisa ithagethi endaweni engenalutho.Phakathi nayo yonke i-6 ns laser pulse, i-plasma iyaqhubeka nokushisa, ikakhulukazi ngenxa yenqubo ye-bremsstrahlung ephambene.Njengoba ingekho insimu yangaphandle evalekile esetshenziswayo phakathi nesigaba sokushisa, i-plasma iqala ukwanda ngezilinganiso ezintathu.Lapho i-plasma iqala ukwanda phezu kwendawo ehlosiwe, isikhungo sesisindo se-plasma sithola isivinini esibheke endaweni eqondiwe ngamandla angu-600 eV/n.Ngemuva kokushisa, i-plasma iyaqhubeka nokuhamba ohlangothini lwe-axial kusukela ekuhlosweni, ikhula nge-isotropically.
Njengoba kuboniswe kuMfanekiso 2, i-plasma yokukhipha inweba ibe yivolumu yevacuum ezungezwe isiqukathi sensimbi esinamandla afanayo nalawo ahlosiwe.Ngakho-ke, i-plasma ikhukhuleka esifundeni esingenayo insimu iye ku-accelerator ye-RFQ.Inkambu kazibuthe ye-axial isetshenziswa phakathi kwegumbi le-laser irradiation kanye ne-RFQ linac kusetshenziswa inxeba lekhoyili ye-solenoid ezungeze igumbi le-vacuum.Inkambu kazibuthe ye-solenoid icindezela ukunwetshwa kwe-radial kwe-plasma ekhukhulekayo ukuze kugcinwe ukuminyana okuphezulu kwe-plasma phakathi nokulethwa endaweni yokuvula i-RFQ.Ngakolunye uhlangothi, i-plasma iyaqhubeka nokukhula ohlangothini lwe-axial ngesikhathi sokukhukhuleka, yakha i-plasma emide.Ukuchema kwamandla kagesi aphezulu kusetshenziswa emkhunjini wensimbi oqukethe i-plasma ephambi kwembobo yokuphuma endaweni yokungena ye-RFQ.I-voltage echema ikhethiwe ukuze inikeze izinga lomjovo elingu-7Li3+ elidingekayo ukuze i-RFQ linac isheshiswe ngendlela efanele.
I-ablation plasma ewumphumela ayiqukethe kuphela i-7Li3+, kodwa futhi i-lithium kwezinye izifundazwe zokushaja nezinto ezingcolisayo, ezithuthelwa kanyekanye ku-RFQ linear accelerator.Ngaphambi kokuhlolwa okusheshisiwe kusetshenziswa i-RFQ linac, ukuhlaziya isikhathi esingaxhunyiwe ku-inthanethi sendiza (TOF) kwenziwa ukuze kufundwe ukwakheka nokusatshalaliswa kwamandla kwama-ion ku-plasma.Ukusethwa kokuhlaziya okunemininingwane kanye nokusabalalisa kwezindleko zezwe kuchazwe esigabeni Sezindlela.Ukuhlaziywa kubonise ukuthi i-7Li3 + ion yayiyizinhlayiya eziyinhloko, ezibala cishe i-54% yazo zonke izinhlayiya, njengoba kuboniswe kumfanekiso 3. Ngokusho kokuhlaziywa, i-7Li3 + ion yamanje endaweni yokuphuma kwe-ion beam ilinganiselwa ku-1.87 mA.Ngesikhathi sokuhlolwa okusheshisiwe, inkambu ye-solenoid engu-79 mT isetshenziswa ku-plasma ekhulayo.Ngenxa yalokho, i-7Li3+ yamanje ekhishwe ku-plasma futhi ebonwa kumtshina inyuke nge-factory engu-30.
Izingxenyana zama-ion kuplasma ekhiqizwe nge-laser ezitholwe ngokuhlaziywa kwesikhathi sendiza.I-7Li1+ ne-7Li2+ ion yenza u-5% no-25% we-ion beam, ngokulandelana.Ingxenye etholiwe yezinhlayiya ze-6Li ivumelana nokuqukethwe kwemvelo kwe-6Li (7.6%) kuthagethi ye-lithium foil ngaphakathi kwephutha lokuhlola.Ukungcoliswa komoyampilo okuncane (6.2%) kwabonwa, ikakhulukazi i-O1+ (2.1%) kanye ne-O2+ (1.5%), okungenzeka kube ngenxa yokukhishwa kwe-oxidation ebusweni bethagethi ye-lithium foil.
Njengoba kushiwo ngaphambili, i-lithium plasma ikhukhuleka endaweni engenamasimu ngaphambi kokungena ku-RFQ linac.Okokufaka kwe-linac ye-RFQ kunembobo yobubanzi obungu-6 mm esitsheni sensimbi, futhi i-voltage echema ingu-52 kV.Nakuba amandla kagesi e-RFQ eshintsha ngokushesha ±29 kV ku-100 MHz, i-voltage ibangela ukushesha kwe-axial ngoba ama-electrode e-RFQ accelerator anesilinganiso samandla anguziro.Ngenxa yenkambu kagesi eqinile ekhiqizwe kugebe elingu-10 mm phakathi kwesimbobo kanye nonqenqema lwe-electrode ye-RFQ, ama-ion e-plasma e-positive kuphela akhishwa ku-plasma endaweni evulekayo.Ezinhlelweni zendabuko zokulethwa kwe-ion, ama-ion ahlukaniswa ne-plasma ngendawo kagesi ebangeni elide phambi kwesisheshisi se-RFQ bese igxiliswa endaweni yokuvula i-RFQ ngento egxilile ye-beam.Kodwa-ke, ngenxa yemishayo ye-ion esindayo eqinile edingekayo kumthombo oqinile we-neutron, amandla anyanyekayo angewona umugqa ngenxa yemiphumela yokushaja kwesikhala angaholela ekulahlekelweni okuphawulekayo kwamanje kwe-ion ohlelweni lwezokuthutha lwe-ion, kukhawule umthamo wamanje ongasheshiswa.Ku-DPIS yethu, ama-ion anamandla amakhulu athuthwa njenge-plasma ekhukhulekayo ngqo endaweni yokuphuma yembobo ye-RFQ, ngakho-ke akukho ukulahleka kwe-ion beam ngenxa yokushajwa kwesikhala.Phakathi nalokhu kuboniswa, i-DPIS yasetshenziswa kugongolo lwe-lithium-ion okokuqala ngqa.
Isakhiwo se-RFQ sathuthukiselwa ukugxila kanye nokusheshisa imishayo ye-ion yamanje yamandla aphansi futhi isibe indinganiso yokusheshisa kwe-oda lokuqala.Sisebenzise i-RFQ ukusheshisa ama-ion angu-7Li3+ ukusuka kumandla okufakelwa angu-22 keV/n kuya ku-204 keV/n.Nakuba i-lithium nezinye izinhlayiya ezine-charge ephansi ku-plasma nazo zikhishwa ku-plasma futhi zifakwe ku-RFQ aperture, i-RFQ linac isheshisa ama-ion kuphela nge-charge-to-mass ratio (Q/A) eduze ne-7Li3+.
Emkhiwaneni.Umfanekiso wesi-4 ubonisa amagagasi atholwe i-transformer yamanje (CT) ekuphumeni kwe-RFQ linac kanye ne-Faraday cup (FC) ngemva kokuhlaziya uzibuthe, njengoba kuboniswe kumfanekiso.2. Ukushintsha kwesikhathi phakathi kwamasignali kungahunyushwa njengomehluko ngesikhathi sokundiza endaweni yomtshina.Isilinganiso se-ion esiphezulu esikalwe ku-CT sasingu-43 mA.Esimweni se-RT, ugongolo olubhalisiwe alukwazi ukuqukatha ama-ion asheshiselwe amandla abaliwe kuphela, kodwa nama-ion ngaphandle kwe-7Li3+, angasheshisi ngokwanele.Kodwa-ke, ukufana kwamafomu amanje e-ion atholakala ngokusebenzisa i-QD ne-PC kubonisa ukuthi i-ion yamanje ngokuyinhloko iqukethe i-7Li3+ esheshayo, futhi ukwehla kwenani eliphakeme lamanje ku-PC kubangelwa ukulahlekelwa kwensimbi ngesikhathi sokudluliselwa kwe-ion phakathi kwe-QD ne-QD. I-PC.Ukulahlekelwa Lokhu kuqinisekiswa futhi ukulingiswa kwemvilophu.Ukulinganisa ngokunembile umthamo wamanje we-7Li3+, ugongolo luhlaziywa ngozibuthe we-dipole njengoba kuchazwe esigabeni esilandelayo.
Ama-oscillograms we-beam esheshisiwe aqoshwe endaweni yomtshina i-CT (ijika elimnyama) ne-FC (ijika elibomvu).Lezi zilinganiso ziqalwa ukutholwa kwemisebe ye-laser yisithwebuli sezithombe ngesikhathi sokukhiqizwa kwe-laser plasma.Ijika elimnyama libonisa i-waveform elinganiswa ku-CT exhunywe kokuphumayo kwe-linac ye-RFQ.Ngenxa yokuba seduze kwe-RFQ linac, umtshina uthatha umsindo we-100 MHz RF, ngakho-ke kwasetshenziswa isihlungi se-FFT esingu-98 MHz esisezingeni eliphansi ukuze sikhiphe isignali ye-RF ye-resonant engu-100 MHz ebekwe phezulu kusiginali yokuthola.Ijika elibomvu likhombisa i-waveform ku-FC ngemuva kokuthi uzibuthe ohlaziyayo eqondise ugongolo lwe-ion lwe-7Li3+.Kulo mkhakha kazibuthe, ngaphandle kwe-7Li3+, N6+ ne-O7+ ingathuthwa.
I-ion beam ngemva kwe-RFQ linac igxile ochungechungeni lwezibuthe ezintathu ezigxiliswe yi-quadrupole bese ihlaziywa ngozibuthe be-dipole ukuze kuhlukaniswe ukungcola ku-ion beam.Inkambu kazibuthe engu-0.268 T iqondisa imishayo engu-7Li3+ ku-FC.I-waveform yokuthola yale nkundla kazibuthe iboniswa njengejiko elibomvu kuMfanekiso 4. I-wave ephakeme kakhulu yamanje ifinyelela ku-35 mA, ephakeme izikhathi ezingaphezu kweziyi-100 kune-Li3+ evamile ekhiqizwa kuma-accelerator akhona avamile ka-electrostatic.Ububanzi be-beam pulse bungu-2.0 µs ngobubanzi obugcwele kuhhafu wobukhulu.Ukutholwa kwesigxobo se-7Li3+ esinensimu kazibuthe ye-dipole kukhombisa ukunqwabelana okuphumelelayo nokusheshisa kwe-beam.I-ion beam yamanje etholwe yi-FC lapho iskena inkambu kazibuthe ye-dipole iboniswa ku-Fig. 5. Kubonwe ukuphakama okukodwa okuhlanzekile, okuhlukaniswe kahle kwezinye iziqongo.Njengoba wonke ama-ion asheshiselwa kumandla okuklama i-RFQ linac enejubane elifanayo, ama-ion ama-ion ane-Q/A efanayo kunzima ukuwahlukanisa ngamasimu kazibuthe e-dipole.Ngakho-ke, asikwazi ukuhlukanisa i-7Li3+ ku-N6+ noma i-O7+.Kodwa-ke, inani lokungcola lingalinganiselwa ezifundazweni ezikhokhiswayo ezingomakhelwane.Isibonelo, i-N7+ ne-N5+ zingahlukaniswa kalula, kuyilapho i-N6+ ingase ibe yingxenye yokungcola futhi kulindeleke ukuthi ibe khona cishe ngenani elifanayo ne-N7+ ne-N5+.Izinga lokungcola elilinganiselwe lilinganiselwa ku-2%.
I-spectra yengxenye ye-Beam etholwe ngokuskena inkambu kazibuthe ye-dipole.Isilinganiso esiphezulu ku-0.268 T sihambisana ne-7Li3+ ne-N6+.Ububanzi be-peak buncike kusayizi we-beam ekusikeni.Naphezu kweziqongo ezibanzi, i-7Li3+ ihlukanisa kahle ne-6Li3+, O6+, ne-N5+, kodwa ihlukana kabi ne-O7+ ne-N6+.
Endaweni ye-FC, iphrofayili ye-beam yaqinisekiswa nge-plug-in scintillator futhi yaqoshwa ngekhamera yedijithali esheshayo njengoba kuboniswe kuMfanekiso 6. I-7Li3+ pulsed beam ene-current ye-35 mA iboniswa ukuthi isheshiselwe ku-RFQ ebaliwe. amandla angu-204 keV/n, ahambisana ne-1.4 MeV, futhi adluliselwe kumtshina we-FC.
Iphrofayela ye-Beam ibonwe esikrinini se-pre-FC scintillator (enemibala yi-Fiji, 2.3.0, https://imagej.net/software/fiji/).Inkambu kazibuthe kazibuthe we-dipole ehlaziyayo yashunwa ukuze iqondise ukusheshisa kwe-Li3+ ion beam ku-RFQ yamandla okuklama.Amachashazi aluhlaza okwesibhakabhaka endaweni eluhlaza abangelwa impahla ye-scintillator enesici.
Sizuze ukukhiqizwa kwama-ion angu-7Li3+ ngokukhipha i-laser ebusweni be-lithium foil eqinile, futhi ugongolo lwamanje lwe-ion oluphezulu lwabanjwa futhi lwasheshiswa nge-RFQ linac eklanywe ngokukhethekile kusetshenziswa i-DPIS.Kumandla we-1.4 MeV, ukuphakama okuphezulu kwe-7Li3+ kufinyelelwe ku-FC ngemuva kokuhlaziywa kukazibuthe bekungama-35 mA.Lokhu kuqinisekisa ukuthi ingxenye ebaluleke kakhulu yokuqaliswa komthombo we-neutron nge-kinematics ephambene isetshenziswe ngokuhlola.Kule ngxenye yephepha, kuzoxoxwa ngakho konke ukuklama komthombo we-neutron ehlangene, okuhlanganisa ama-accelerator aphezulu kanye neziteshi eziqondiswe yi-neutron.Umklamo usekelwe emiphumeleni etholwe ngamasistimu akhona elabhorethri yethu.Kufanele kuqashelwe ukuthi ukuphakama okuphezulu kwe-ion beam kungandiswa ngokuqhubekayo ngokunciphisa ibanga phakathi kwe-lithium foil ne-RFQ linac.Ilayisi.7 ubonisa wonke umqondo womthombo we-neutron ehlangene ohlongozwayo ku-accelerator.
Idizayini yomqondo yomthombo we-neutron ehlangene ohlongozwayo ku-accelerator (edwetshwe yi-Freecad, 0.19, https://www.freecadweb.org/).Ukusuka kwesokudla kuye kwesobunxele: umthombo we-laser ion, uzibuthe we-solenoid, i-RFQ linac, ukudluliswa kwe-medium energy beam (MEBT), i-IH linac, negumbi lokusebenzisana lokukhiqiza i-neutron.Ukuvikelwa kwemisebe kunikezwa ngokuyinhloko ekuqondeni phambili ngenxa yemvelo eqondiswe kancane yemishayo ye-neutron ekhiqiziwe.
Ngemuva kwe-RFQ linac, kuhlelwa ukusheshisa okwengeziwe kwe-Inter-digital H-structure (IH linac)30 linac.Ama-linacs e-IH asebenzisa isakhiwo seshubhu lokukhukhuleka i-π-mode ukuze anikeze ama-gradient enkambu kagesi aphezulu phezu kohlu oluthile lwezivinini.Ucwaningo lomqondo lwenziwa ngokususelwa ku-1D longitudinal dynamics simulation kanye nokulingiswa kwegobolondo le-3D.Izibalo zibonisa ukuthi i-100 MHz IH linac ene-voltage ye-drift drift enengqondo (engaphansi kuka-450 kV) kanye nozibuthe ogxilile oqinile ingasheshisa i-40 mA beam isuka ku-1.4 iye ku-14 MeV ebangeni elingu-1.8 m.Ukusatshalaliswa kwamandla ekupheleni kweketango le-accelerator kulinganiselwa ku-± 0.4 MeV, okungathinti kakhulu i-spectrum yamandla e-neutron ekhiqizwa yithagethi yokuguqula i-neutron.Ngaphezu kwalokho, ukukhishwa kwe-beam kuphansi ngokwanele ukuze kugxiliswe i-beam endaweni encane ye-beam kunalokho obekungadingeka ngokuvamile ukuze uthole amandla aphakathi nendawo kanye nosayizi we-quadrupole magnet.Ekudluliselweni kwe-medium energy beam (MEBT) phakathi kwe-RFQ linac ne-IH linac, i-beamforming resonator isetshenziselwa ukunakekela ukwakheka kwe-beamforming.Ozibuthe abathathu abangama-quadrupole basetshenziswa ukulawula usayizi we-beam eseceleni.Lelisu lokuklama lisetshenziswe kuma-accelerator amaningi31,32,33.Ubude obuphelele balo lonke uhlelo ukusuka emthonjeni we-ion kuya ekamelweni eliqondiwe bulinganiselwa ukuthi bungaphansi kwamamitha angu-8, obungangena elolini elivamile le-semi-trailer.
Ithagethi yokuguqula i-neutron izofakwa ngqo ngemva kwesisheshisi somugqa.Sixoxa ngemiklamo yesiteshi esiqondiswe kuyo ngokusekelwe ezifundweni ezedlule sisebenzisa izimo ze-kinematic eziphambene23.Okuhlosiwe okubikiwe kokuguqulwa kufaka phakathi izinto eziqinile (i-polypropylene (C3H6) ne-titanium hydride (TiH2)) kanye nezinhlelo eziqondiwe zegesi.Umgomo ngamunye unezinzuzo kanye nokubi.Okuqondiwe okuqinile kuvumela ukulawula ukujiya okunembe.Ukuncipha kwethagethi, kulapho kunembe kakhulu ukuhlelwa kwendawo kokukhiqizwa kwe-neutron.Nokho, lokho okuhlosiwe kusengase kube nezinga elithile lokusabela kwenuzi okungafunwa kanye nemisebe.Ngakolunye uhlangothi, i-hydrogen target inganikeza indawo ehlanzekile ngokuqeda ukukhiqizwa kwe-7Be, umkhiqizo oyinhloko we-nuclear reaction.Kodwa-ke, i-hydrogen inekhono lokuvimba elibuthakathaka futhi idinga ibanga elikhulu lomzimba ukuze kukhishwe amandla anele.Lokhu kubi kancane ezilinganisweni ze-TOF.Ukwengeza, uma ifilimu encane isetshenziselwa ukuvala i-hydrogen target, kuyadingeka ukucabangela ukulahlekelwa kwamandla emisebe ye-gamma ekhiqizwa ifilimu encane kanye nesigameko se-lithium beam.
I-LICORNE isebenzisa okuqondiwe kwe-polypropylene futhi isistimu eqondiwe ithuthukiselwe kumaseli e-hydrogen avalwe nge-tantalum foil.Uma kubhekwa i-beam current engu-100 nA ye-7Li34, zombili izinhlelo eziqondiwe zingakhiqiza kufika ku-107 n/s/sr.Uma sisebenzisa lokhu kuguqulwa kwesivuno senutroni esifunwayo emthonjeni wethu we-neutron ohlongozwayo, khona-ke i-lithium eshayelwa yi-lithium engu-7 × 10–8 C ingatholwa ngomshini we-laser ngamunye.Lokhu kusho ukuthi ukudubula i-laser kabili nje ngomzuzwana kukhiqiza ama-neutron angama-40% ngaphezu kwalokho i-LICORNE engakhiqiza ngomzuzwana owodwa ngomsebe oqhubekayo.Ukuguquguquka okuphelele kungakhuliswa kalula ngokwandisa imvamisa yokuvusa ye-laser.Uma sicabanga ukuthi kukhona isistimu yelaser engu-1 kHz emakethe, ukugeleza kwe-neutron okumaphakathi kungakhuliswa kalula kufike ku-7 × 109 n/s/sr.
Uma sisebenzisa amasistimu wezinga eliphezulu lokuphindaphinda ngezinhloso zepulasitiki, kuyadingeka ukulawula ukukhiqizwa kokushisa kokuhlosiwe ngoba, isibonelo, i-polypropylene inephuzu elincibilikayo eliphansi lika-145-175 ° C kanye ne-thermal conductivity ephansi engu-0.1-0.22 W/ m/K.Ngebhimu ye-lithium-ion engu-14 MeV, ithagethi ye-polypropylene ewugqinsi engu-7 µm yanele ukunciphisa amandla ebhimu kumkhawulo wokusabela (13.098 MeV).Uma kucatshangelwa umphumela ophelele wama-ion okhiqizwe i-laser shot eyodwa kokuhlosiwe, ukukhululwa kwamandla e-lithium ion nge-polypropylene kulinganiselwa ku-64 mJ/i-pulse.Uma sicabanga ukuthi wonke amandla adluliswa kuyindilinga enobubanzi obuyi-10 mm, ishayela ngalinye lihambisana nokukhuphuka kwezinga lokushisa okungaba ngu-18 K/pulse.Ukukhishwa kwamandla kokuhlosiwe kwe-polypropylene kusekelwe ekucabangeni okulula kokuthi konke ukulahlekelwa kwamandla kugcinwa njengokushisa, ngaphandle kwemisebe noma okunye ukulahlekelwa ukushisa.Njengoba ukukhulisa inani lama-pulses ngesekhondi ngalinye kudinga ukuqedwa kokwanda kokushisa, singasebenzisa okuqondiwe kwe-strip ukugwema ukukhishwa kwamandla endaweni efanayo23.Uma sithatha indawo ye-10 mm ye-beam kokuqondisiwe enezinga lokuphinda i-laser elingu-100 Hz, isivinini sokuskena setheyiphu ye-polypropylene singaba ngu-1 m/s.Izilinganiso eziphakeme zokuphindaphinda zingenzeka uma ukugqagqana kwendawo ye-beam kuvunyelwe.
Siphinde saphenya okuhlosiwe ngamabhethri e-hydrogen, ngoba imishayo yokushayela enamandla ingasetshenziswa ngaphandle kokulimaza okuhlosiwe.I-neutron beam ingalungiswa kalula ngokushintsha ubude bekamelo legesi kanye nokucindezela kwe-hydrogen ngaphakathi.Amafoil ensimbi azacile avame ukusetshenziswa kuma-accelerator ukuze ahlukanise indawo enegesi yethagethi ku-vacuum.Ngakho-ke, kuyadingeka ukwandisa amandla wesigameko se-lithium-ion beam ukuze kunxeshezelwe ukulahlekelwa kwamandla ku-foil.Ukuhlanganiswa okuhlosiwe okuchazwe embikweni 35 kwakuhlanganisa isiqukathi se-aluminium esingu-3.5 cm ubude nomfutho wegesi we-H2 ongu-1.5 atm.I-16.75 MeV lithium ion beam ingena ebhethrini ngefoil ye-Ta epholile engu-2.7 µm, futhi amandla we-lithium ion beam ekugcineni kwebhethri ancishiselwa ku-threshold yokusabela.Ukuze kwandiswe amandla e-beam amabhethri e-lithium-ion asuka ku-14.0 MeV aye ku-16.75 MeV, i-IH linac kwakudingeka inwetshwe cishe ngo-30 cm.
Ukukhishwa kwama-neutron kusuka ekuqondisweni kweseli yegesi nakho kwacwaningwa.Mayelana nokuhlosiwe kwegesi ye-LICORNE okukhulunywe ngayo ngenhla, ukulingiswa kwe-GEANT436 kubonisa ukuthi ama-neutron agxile kakhulu akhiqizwa ngaphakathi kwekhoni, njengoba kuboniswe kuMfanekiso 1 ku-[37].Ireferensi engu-35 ikhombisa ububanzi bamandla ukusuka ku-0.7 kuye ku-3.0 MeV ngokuvuleka kwekhoni okuphezulu okungu-19.5° ngokuhlobene nendlela yokusatshalaliswa kwe-beam eyinhloko.Ama-neutron agxile kakhulu anganciphisa kakhulu inani lezinto ezivikelayo kuma-engeli amaningi, ehlise isisindo sesakhiwo futhi anikeze ukuguquguquka okukhulu ekufakweni kwemishini yokulinganisa.Ngokombono wokuvikelwa kwemisebe, ngaphezu kwama-neutron, le thagethi yegesi ikhipha imisebe ye-gamma engu-478 keV isotropically ohlelweni lwe-centroid coordinate38.Le misebe ye-γ ikhiqizwa ngenxa ye-7Be decay kanye ne-7Li deexcitation, okwenzeka lapho i-Li beam eyinhloko ishaya iwindi lokufaka elithi Ta.Nokho, ngokwengeza i-cylindrical cylindrical collimator engu-35 Pb/Cu ewugqinsi, ingemuva lingancishiswa kakhulu.
Njengenye inhloso, umuntu angasebenzisa ifasitela le-plasma [39, 40], okwenza kube nokwenzeka ukufeza ukucindezela kwe-hydrogen ephakeme kakhulu kanye nesifunda esincane sendawo yokukhiqiza i-neutron, nakuba ingaphansi kwezinhloso eziqinile.
Siphenya izinketho zokukhomba ukuguqulwa kwe-neutron zokusabalalisa amandla okulindelekile kanye nosayizi we-beam we-lithium ion beam kusetshenziswa i-GEANT4.Ukulingiswa kwethu kubonisa ukusatshalaliswa okungaguquki kwamandla enutroni kanye nokusabalalisa kwe-angular kokuhlosiwe kwe-hydrogen ezincwadini ezingenhla.Kunoma iyiphi isistimu eqondiwe, ama-neutron agxile kakhulu angakhiqizwa ukusabela kwe-kinematic okuphambene okuqhutshwa ugongolo oluqinile lwe-7Li3+ kuthagethi ecebile nge-hydrogen.Ngakho-ke, imithombo emisha ye-neutron ingasetshenziswa ngokuhlanganisa ubuchwepheshe obuvele bukhona.
Izimo ze-laser irradiation zikhiqize kabusha ukuhlolwa kokukhiqizwa kwe-ion beam ngaphambi kokuboniswa okusheshisiwe.I-laser iwuhlelo lwedeskithophu i-nanosecond Nd:YAG enamandla okuminyana kwe-laser angu-1012 W/cm2, ubude begagasi obuyisisekelo obungu-1064 nm, indawo yamandla engu-800 mJ, kanye nobude be-pulse obungu-6 ns.Ububanzi bendawo kokuqondisiwe bulinganiselwa ku-100 µm.Ngenxa yokuthi insimbi ye-lithium (i-Alfa Aesar, i-99.9% ehlanzekile) ithambile impela, izinto ezisikwe kahle zicindezelwa esikhunjeni.Ubukhulu be-foil 25 mm × 25 mm, ukujiya 0.6 mm.Ukulimala okufana ne-crater kwenzeka endaweni eqondiwe lapho i-laser ilishaya, ngakho okuqondiwe kushukunyiswa inkundla enenjini ukuze kuhlinzekwe ingxenye entsha yendawo okuqondiwe kuyo ngeshothi ye-laser ngayinye.Ukuze ugweme ukuhlanganiswa kabusha ngenxa yegesi esele, ukucindezela ekamelweni kwakugcinwe ngaphansi kwebanga le-10-4 Pa.
Ivolumu yokuqala ye-laser plasma incane, njengoba ubukhulu bendawo ye-laser buyi-100 μm futhi phakathi kwama-6 ns ngemva kokukhiqizwa kwayo.Ivolumu ingathathwa njengephuzu eliqondile futhi inwetshwe.Uma umtshina ubekwe ebangeni xm ukusuka endaweni okuqondiwe kuyo, isignali eyamukelwe ilalela ubudlelwano: i-ion yamanje I, isikhathi sokufika se-ion t, nobubanzi be-pulse τ.
I-plasma ekhiqiziwe yacwaningwa ngendlela ye-TOF nge-FC kanye ne-energy ion analyzer (EIA) etholakala ebangeni elingu-2.4 m no-3.85 m ukusuka ku-laser target.I-FC inegridi yokucindezela echemile ngo -5 kV ukuvimbela ama-electron.I-EIA ine-deflector engu-90 degree electrostatic ehlanganisa ama-electrode amabili ensimbi ayi-coaxial cylindrical anevoltheji efanayo kodwa ephambene, eqondile ngaphandle futhi engemihle ngaphakathi.I-plasma ekhulayo iqondiswe ku-deflector ngemuva kwe-slot futhi iphambukiswe insimu kagesi edlula kusilinda.Ama-ion anelisa ubudlelwano E/z = i-eKU itholwa kusetshenziswa i-Secondary Electron Multiplier (SEM) (Hamamatsu R2362), lapho u-E, z, e, K, no-U okungamandla e-ion, isimo sokushaja, kanye nokushaja kuyizici ze-EIA zejometri. .ama-electron, ngokulandelana, kanye nomehluko ongaba khona phakathi kwama-electrode.Ngokushintsha i-voltage kuyo yonke i-deflector, umuntu angathola amandla nokusatshalaliswa kwe-ion ku-plasma.I-voltage yokushanela i-U/2 EIA ikububanzi obusuka ku-0.2 V ukuya ku-800 V, obuhambisana namandla e-ion ebangeni elisuka ku-4 eV ukuya ku-16 keV esimweni sokushaja ngasinye.
Ukusatshalaliswa kwesimo sokushaja sama-ion ahlaziywa ngaphansi kwemibandela ye-laser irradiation echazwe esigabeni esithi "Isizukulwane semishayo ye-lithium ehlutshiwe ngokugcwele" kuboniswa ku-Fig.8.
Ukuhlaziywa kokusatshalaliswa kwesimo sokukhokha sama-ion.Nansi iphrofayela yesikhathi sokuminyana yamanje ye-ion ehlaziywe nge-EIA yase ikalwa ku-1 m ukusuka kucwecwe lwe-lithium kusetshenziswa isibalo.(1) kanye (2).Sebenzisa izimo ze-laser irradiation ezichazwe esigabeni esithi "Isizukulwane Se-Lithium Beam Ekhishwe Ngokuphelele".Ngokuhlanganisa ukuminyana ngakunye kwamanje, inani lama-ion ku-plasma libalwe, eliboniswe kuMfanekiso 3.
Imithombo ye-Laser ion ingaletha ugongolo lwe-ion lwe-multi-mA olunamandla ngokushaja okuphezulu.Kodwa-ke, ukulethwa kwe-beam kunzima kakhulu ngenxa yokuxoshwa kwe-space charge, ngakho-ke akuzange kusetshenziswe kabanzi.Kuhlelo lwendabuko, imishayo ye-ion ikhishwa ku-plasma futhi ithuthelwe ku-accelerator eyinhloko ngomugqa we-boam onamazibuthe amaningana agxilile ukuze alolonge ugongolo lwe-ion ngokuya nekhono lokuthatha lesisheshisi.Emisebeni yamandla eshaja emkhathini, imishayo iyahluka ngokungaqondile, futhi ukulahlekelwa okukhulu kwemishayo kuyabonwa, ikakhulukazi endaweni yesivinini esiphansi.Ukuze kunqotshwe le nkinga ekuthuthukisweni kwama-accelerator ekhabhoni yezokwelapha, kuhlongozwa uhlelo olusha lokulethwa kwe-DPIS41.Sisebenzise le nqubo ukusheshisa i-lithium-ion beam enamandla kusuka emthonjeni omusha we-neutron.
Njengoba kuboniswe emkhiwaneni.4, indawo lapho i-plasma ikhiqizwa futhi yandiswa khona izungezwe isitsha sensimbi.Isikhala esivalekile sifinyelela ekungeneni kweresonator ye-RFQ, okuhlanganisa nevolumu engaphakathi kwekhoyili ye-solenoid.Kufakwe amandla kagesi angu-52 kV esitsheni.Ku-resonator ye-RFQ, ama-ion adonswa ngamandla ngembobo engu-6 mm ububanzi ngokumisa i-RFQ.Amandla aphikisayo angenawo umugqa emugqeni womugqa ayasuswa njengoba ama-ion ethuthwa kusimo se-plasma.Ngaphezu kwalokho, njengoba kushiwo ngenhla, sisebenzise inkambu ye-solenoid ngokuhlanganisa ne-DPIS ukuze silawule futhi sikhulise ukuminyana kwama-ion endaweni yokukhipha imbobo.
I-accelerator ye-RFQ iqukethe i-cylindrical vacuum chamber njengoba kuboniswe kumfanekiso.9a.Ngaphakathi kwayo, izinduku ezine zethusi ezingenawo umoya-mpilo zibekwe i-quadrupole-symmetrically ezungeze i-axis ye-beam (Fig. 9b).Izinduku ezi-4 namagumbi akha isekethe ye-RF ezwakalayo.Inkambu ye-RF ekhangisiwe idala i-voltage eshintsha isikhathi kuyo yonke intonga.Ama-ion atshalwe ngobude azungeze i-eksisi abanjwe eceleni yinkundla ye-quadrupole.Ngesikhathi esifanayo, iphoyinti lenduku lilungiswa ukuze lidale insimu kagesi ye-axial.Inkambu ye-axial ihlukanisa i-beam eqhubekayo ejovwe ibe uchungechunge lwezinsimbi ze-beam ezibizwa ngokuthi i-beam.Uhlaka ngalunye luqukethwe phakathi nesikhathi esithile somjikelezo we-RF (10 ns).Imishayo eseduze ihlukaniswa ngokwenkathi yefrikhwensi yomsakazo.Ku-RFQ linac, i-2 µs beam ephuma emthonjeni we-laser ion iguqulwa ibe ukulandelana kwemishayo engama-200.Ugongolo lube selusheshiselwa emandleni abaliwe.
I-RFQ yesisheshisi somugqa.(a) (kwesokunxele) Ukubuka kwangaphandle kwe-RFQ linac chamber.(b) (kwesokudla) I-electrode enezinduku ezine ekamelweni.
Imingcele yokuklama eyinhloko ye-RFQ linac amandla kagesi wenduku, imvamisa ye-resonant, i-beam hole radius, kanye nokushintshwa kwe-electrode.Khetha i-voltage entweni engu-± 29 kV ukuze indawo kagesi ibe ngaphansi komkhawulo wokuwohloka kukagesi.Lapho imvamisa ye-resonant iphansi, amandla okugxila asemaceleni aba makhulu kanye nenkambu yokusheshisa emaphakathi.I-aperture radii enkulu yenza kube nokwenzeka ukukhulisa usayizi we-beam futhi, ngenxa yalokho, kwandiswe i-beam yamanje ngenxa yokwehliswa kwenkokhelo yesikhala esincane.Ngakolunye uhlangothi, i-aperture radii emikhulu idinga amandla e-RF engeziwe ukuze inike amandla i-RFQ linac.Ngaphezu kwalokho, kunqunyelwe izidingo zekhwalithi zesayithi.Ngokusekelwe kulawa mabhalansi, imvamisa ye-resonant (100 MHz) kanye ne-aperture radius (4.5 mm) zikhethelwe ukusheshisa kwe-high-current beam.I-modulation ikhethwa ukuze kuncishiswe ukulahleka kwe-beam futhi kukhuphule ukusheshisa ukusebenza kahle.Idizayini ithuthukiswe izikhathi eziningi ukuze ikhiqize umklamo we-RFQ linac ongasheshisa ama-ion angu-7Li3+ ku-40 mA ukusuka ku-22 keV/n kuya ku-204 keV/n phakathi kwamamitha angu-2.Amandla e-RF akalwa ngesikhathi sokuhlolwa ayengu-77 kW.
Ama-linacs e-RFQ angasheshisa ama-ion ngobubanzi obuthile be-Q/A.Ngakho-ke, lapho uhlaziya i-beam ephakelwayo kuze kube sekupheleni kwe-accelerator eqondile, kubalulekile ukucabangela ama-isotopes nezinye izinto.Ngaphezu kwalokho, ama-ion afunwayo, asheshiswe kancane, kodwa ehle ngaphansi kwezimo zokusheshisa phakathi kwe-accelerator, asengakwazi ukuhlangabezana nokuvalelwa kwe-lateral futhi angathuthwa aze afike ekugcineni.Imisebe engadingeki ngaphandle kwezinhlayiya ezakhiwe ngo-7Li3+ ibizwa ngokuthi ukungcola.Ekuhloleni kwethu, ukungcola kwe-14N6+ kanye ne-16O7+ kwakuyizinto ezikhathazayo kakhulu, njengoba i-lithium metal foil isabela nge-oxygen ne-nitrogen emoyeni.Lawa ma-ion anesilinganiso se-Q/A esingasheshiswa ngo-7Li3+.Sisebenzisa izibuthe ze-dipole ukuze sihlukanise imishayo yekhwalithi ehlukile nekhwalithi yokuhlaziywa kwe-beam ngemva kwe-RFQ linac.
Ulayini we-beam ngemva kwe-RFQ linac yakhelwe ukuletha ugongolo olusheshiswe ngokugcwele lwe-7Li3+ ku-FC ngemva kukazibuthe we-dipole.-400 V ama-electrode asetshenziselwa ukucindezela ama-electron esibili enkomishini ukuze kulinganiswe ngokunembile umthamo wamanje we-ion.Ngalawa ma-optics, ama-ion trajectories ahlukaniswa abe ama-dipoles futhi agxile ezindaweni ezihlukene kuye nge-Q/A.Ngenxa yezici ezihlukahlukene ezifana nokusabalala komfutho kanye nokuhlehla kokushaja kwesikhala, i-beam ekugxilweni kwayo inobubanzi obuthile.Uhlobo lungahlukaniswa kuphela uma ibanga eliphakathi kwezindawo okugxilwe kuzo zezinhlobo ezimbili ze-ion likhulu kunobubanzi be-beam.Ukuze uthole ukulungiswa okuphezulu kakhulu, i-slit evundlile ifakwa eduze nokhalo lwe-beam, lapho ugongolo lugxile khona.Isikrini se-scintillation (CsI(Tl) esivela e-Saint-Gobain, 40 mm × 40 mm × 3 mm) sifakwe phakathi kokusikeka ne-PC.I-scintillator yasetshenziswa ukuze kutholwe ukuhlukana okuncane kakhulu izinhlayiya eziklanyelwe okwakudingeka zidlule kukho ukuze zilungiswe kahle futhi zibonise osayizi abamukelekayo bemishayo yemishayo ye-ion esindayo ephezulu yamanje.Isithombe se-beam ku-scintillator sirekhodwa ikhamera ye-CCD ngefasitela le-vacuum.Lungisa iwindi lesikhathi sokuchayeka ukuze limboze bonke ububanzi be-beam pulse.
Amasethi edatha asetshenzisiwe noma ahlaziywa ocwaningweni lwamanje ayatholakala kubabhali abafanele uma kunesicelo esifanele.
UManke, I. et al.Isithombe esinezinhlangothi ezintathu zezizinda kazibuthe.Umhlangano kazwelonke.1, 125. https://doi.org/10.1038/ncomms1125 (2010).
Anderson, IS et al.Amathuba okufunda imithombo ye-neutron ehlangene kuma-accelerator.i-physics.I-Rep. 654, 1-58.https://doi.org/10.1016/j.physrep.2016.07.007 (2016).
Urchuoli, A. et al.I-neutron-based computed microtomography: I-Pliobates cataloniae ne-Barberapithecus huerzeleri njengamakesi okuhlola.Yebo.J. Physics.i-anthropology.166, 987–993.https://doi.org/10.1002/ajpa.23467 (2018).

 


Isikhathi sokuthumela: Mar-08-2023