21.15109/CONCORDA/N6ODFLSzilágyi, EditEditSzilágyi0000-0003-3210-0121HUN-REN Wigner Research Centre for PhysicsPal, Manoj KumarManoj KumarPal0000-0003-2803-7449HUN-REN Wigner Research Centre for PhysicsKótai, EndreEndreKótai7004156294HUN-REN Wigner Research Centre for PhysicsZolnai, ZsoltZsoltZolnai7004111126HUN-REN Centre for Energy ResearchBányász, IstvánIstvánBányász57203479861HUN-REN Wigner Research Centre for PhysicsARP2024PhysicsIonoluminescence; SiO2; Defects; Helium irradiationSzilágyi, EditEditSzilágyiHUN-REN Wigner Research Centre for PhysicsSzilágyi, EditEditSzilágyiHUN-REN Wigner Research Centre for Physics2024-02-052024-07-1610.5158/ARP/N6ODFL10.1016/j.nimb.2024.165470422798733673777379737973657407736674351217824646938181016665284568902327917297406851813276209062722964718982288144787725050644342956204423256732502304793050932379306882662532902329333297233098331573322027110333343129333445334363141233476335093355431471335913147533598336233362333618274792746227456315833368233674316103163731633337093375133725337613373933756275633373833801337693171733780337833383027612338133382733830338453381133820338513383733849276423381833847338143386731772317842763533864338563384433841338373386331773276653383931770338663385433855338493386633887338853383733870317902769333881338803388631824339142768727729338793390433917318202770233895318262768033895318353184433889318583187833926339253187233934339143394731842318603390433931318353391531868318643394331884339583393933953339413392833937277213398431889339653395333976339592776833973339583396433947339783396427749339983394933935339523395933985339743392427758339633399433950339883397333976277513399833965340163396033986339742776033987339543397933980339773397033988319463399233942339673400333997339783400627775319223400531893277533399434014278183399734001319263401434008319513399331947339913401531950340133400634005340122783534009340173400034031340273400627807319893196627834340023402827826278373404333999340243405431946340323403127834340133401634039278263404134022340183404934037278473401134000319643401334026340053196334030319533198027844319662785327820340593404831962340332782331930340262781834022340582785534050340513402934039340383400727850340383402534032278603400727837340133402927859340503402331960340143403034022319493401534022340053403734041278113194634044319793404631955340443403434042278433404431976340293402734045340492785434036340262781434035340293406831970340482782034013278222784034012319833404934064340432784134014319833401834041340403403727826319743198127842340313400133985278173402534006278643403934044319643405434028340253404334040340513405234056319483200634046340223403327854340483403934048320203402534038340563405734060340393405131985319843404632010340823409434044278593407431993340583403934043319603403934037340582784831986340523199234067319773196934090340423402827860319753406532002278553405034074340423405334083340593201234061278823200527840340573407231991340573406534068278543404934083340503405934057340383407327855340463200134052340532785434035340342786534081278633406034085341093408427895340743407534101340763200134094340843201834108279053410134097279222792232051341023412227903340993410034109341122793432066341093416627924341633415627940341713416927987341853208727978341813418834188321343421134218279923420334220279983215628040342433423634256342423425734265342773425728060280823426534301280723222334301343073429834306281122810428125322623433334335343643433934348322943230334360343753229134379322933231234377344013438834423343913441028198343973438528205344143440034411344123440732367344283236634441344462822932371344543445428248344573238934460323823446234450323752826234473344602827234473323963448034467344793447728275344863448834483344752828234487344853241834488282893448534499345023449734492344963451234500324353450034502344973451232455345053450834512345073243834518345083451034509345173450634512345203450632445345173451234511345193452032451345213452934511324513452034524345193452534523283123244934518345282831734522345323451332451283403453234528345252832334521345333452434526345263453632471324592833428336345342832734525345333453234539345343453534531324713453128321283303454034534324673454034534345373454034544324713453732455324593453934545324683246934544283402833334529345373454328340324883455232483324883455934549283443248028335324763454834553283543454732483345423455734556345523454734559345493454734555345443454434545345562835234556345473455234558345573455734553283463455334558345523454828352283413248432495345593249834559345513456334551345533456528361345653456034554345613455434564345613248428351345513455928349345642835734547283433454928342324823454934550345513454834560345603455228352345523455534558345543247828337345483455328358345513248134557324843455428358324903248228357325013456734571345623248334550345553455134565345583455534547324783247828346324833454634553345603453734545283363454134546324703454334549345533455034546345443454234545345483454634544345482833734548345443455234540345293247132460345363453632482345372834034542345363247328337345323453834539345263451728321283273247534543283413452634530345433453934542345503248128331345393248234540345373453228327324693452934528345383452628329345162832834536324553452132441345183453628329345293450928308345213453034519345113451634516324443452228335283302832234520345223452934539345328935994223342939622113176622362216223622162216225622713310622962286227622562236215622362236223622313304622762266224622762286225133136223132246223622362236215621562316225622562251331562256225622362156215621562156215621562176217621762176217621762176215621562156215621562156215621562156215621562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BY-NC 4.0Luminescence is a very powerful tool to analyse various types of defects in a wide range of materials; it is often applied for silica, which is a broadly used material in photonics, microelectronics, nuclear energy industry, optoelectronics and other important technological applications. In this work, a single crystalline (0001) α-SiO₂ (quartz) sample has been investigated by the ionoluminescence (IL) method. In this case, intense emitted light can be observed when a 2 MeV He⁺ beam reaches the quartz sample. Three emission bands were found at 1.45 eV, 1.76 eV and 2.34 eV, the corresponding defects were identified as Si nanoclusters, non-bridging oxygen hole centers (NBOHC), and self-trapped excitons (STEs), respectively. The evolution of the defect related IL peaks was determined as a function of He⁺ irradiation fluence. To perform accurate data evaluation, the instrumental function of the applied IL set-up (collimator, optical fibers and spectrometer) was determined and taken into account. The importance of methodological issues in the IL measurement (including set-up, sample holder and proper beam settings) was also discussed. The described steps of system calibration and data evaluation are indispensable for IL spectrum analysis leading to detailed understanding of defect evolution taking place during the ion beam irradiation process.National Research, Development and Innovation FundK-143263National Research, Development and Innovation FundTKP2021-NVA-03