Àá½Ã¸¸ ±â´Ù·Á ÁÖ¼¼¿ä. ·ÎµùÁßÀÔ´Ï´Ù.

¾ãÀº ¹Ú¸·À» ¾ñÀº TLD ¹ÝÀÀ°¨µµÀÇ ±¤ÀÚ ¿¡³ÊÁö¿¡ ´ëÇÑ ÀÇÁ¸¼º Photon Energy Dependence of the Sensitivity of LiF TLDs Loaded with Thin Material

´ëÇѹæ»ç¼±Á¾¾çÇÐȸÁö 1999³â 17±Ç 3È£ p.256 ~ 260
¹Îº´´Ô, ±è¼ö±æ, ³ëÁرÔ, Á¶¿µ°©,
¼Ò¼Ó »ó¼¼Á¤º¸
¹Îº´´Ô (  ) 
ÀÎÇÏ´ëÇб³ ÀÇ°ú´ëÇÐ ¹æ»ç¼±Á¾¾çÇб³½Ç

±è¼ö±æ (  ) 
°í½Å´ëÇб³ ÀÇÇкΠÀÇ¿¹°ú
³ëÁرԠ(  ) 
ÀÎÇÏ´ëÇб³ ÀÇ°ú´ëÇÐ ¹æ»ç¼±Á¾¾çÇб³½Ç
Á¶¿µ°© (  ) 
ÀÎÇÏ´ëÇб³ ÀÇ°ú´ëÇÐ ¹æ»ç¼±Á¾¾çÇб³½Ç

Abstract

¸ñ Àû : ¾ãÀº ¹Ú¸·À» À§¿¡ ¾ñÀº TLD ¼±·®°èÀÇ ¹ÝÀÀ°ª¿¡ ¿µÇâÀ» ¹ÌÄ¡´Â ÀÎÀÚ¸¦ Á¶»çÇÏ¿´
°í, ƯÈ÷, ±Ý¼Ó ¹Ú¸·À» ¾ñÀº TLD ¼±·®°èÀÇ ±¤ÀÚ¿¡³ÊÁö¿Í Ç¥¸é Èí¼ö¼±·®¿¡ ´ëÇÑ ÀÇÁ¸¼ºÀ»
Á¶»çÇÏ¿´´Ù.
¹æ¹ý ¹× Àç·á : º» ¿¬±¸¿¡¼­´Â TLD-100°ú TLD-100 À§¿¡ ¾ñÀº ¾ãÀº ¹°Áú·Î´Â ÁÖ¼®, ±Ý,
±×¸®°í TE Çöó½ºÆ½ ÆÇÀ» »ç¿ëÇÏ¿´´Ù. °¢ ±Ý¼Ó ¹Ú¸·ÀÇ µÎ²²´Â 0.1 §®, TE Çöó½ºÆ½ ÆÇÀÇ
µÎ²²´Â 1 §®¿´°í °¢ ¹Ú¸·ÀÇ ¸éÀûÀº TLD-100ÀÇ ¸éÀû°ú °°ÀÌ ÇÏ¿´´Ù. ¹æ»ç¼±Ä¡·á¿¡ ¸¹ÀÌ ¾²
ÀÌ´Â 6 MV¿¡¼­ 15 MV»çÀÌÀÇ ±¤ÀÚ¿¡³ÊÁö¿¡ ´ëÇÑ TLD-100ÀÇ ¹ÝÀÀ°¨µµ¿Í ±Ý ¹Ú¸·À» ¾ñÀº
TLD-100ÀÇ ¹ÝÀÀ°¨µµ, ±×¸®°í ÁÖ¼® ¹Ú¸·À» ¾ñÀº TLD-100ÀÇ ¹ÝÀÀ°¨µµ¸¦ ºñ±³ÇØ º¸¾Ò´Ù.
°á °ú : ±Ý¼Ó ¹Ú¸·À» ¾ñÀº TLDÀÇ °æ¿ì Ç¥¸é Èí¼ö¼±·®ÀÇ Áõ°¡°¡ ¸í¹éÈ÷ ³ªÅ¸³ª°í, ±Ý ¹Ú
¸·À» ¾ñÀº TLDÀÇ °æ¿ì 10 MV¿¡¼­ Á¤»ó TLDº¸´Ù ¾à 1.83¹èÁ¤µµ °úÀ× ¹ÝÀÀÇÏ´Â °ÍÀ¸·Î °ü
ÃøµÇ¾úÀ¸¸ç, Èí¼ö¼±·®¿¡ µû¸¥ ¹ÝÀÀ°¨µµÀÇ º¯È­´Â ÁÖ¼®À» ¾ñÀº TLDÀÇ °æ¿ì°¡ °¡Àå ÀÛ¾Ò´Ù.
±Ý¼Ó ¹Ú¸·À» ¾ñÀº TLDÀÇ ÀÏ¹Ý TLD¿¡ ´ëÇÑ »ó´ë ¹ÝÀÀ°¨µµ´Â ¿¡³ÊÁö¿¡ ´ëÇÑ ÀÇÁ¸¼ºÀ» °ÅÀÇ
³ªÅ¸³»Áö ¾Ê¾Ò´Ù. ±×¸®°í ¾ãÀº ¹Ú¸·ÀÇ Á¶Á÷¿¡ ´ëÇÑ µî°¡ µÎ²²¿¡ µû¶ó ¹ÝÀÀ°¨µµ°¡ Áõ°¡ÇÏ¿´
´Ù.
°á ·Ð : ±Ý¼Ó ¹Ú¸·À» ¾ñÀº TLD ¼±·®°èÀÇ ¹ÝÀÀ°ªÀÌ°í ¿¡³ÊÁö(6-15 MV)¿¡ ´ëÇÑ ÀÇÁ¸¼ºÀ»
°ÅÀÇ ³ªÅ¸³»Áö ¾Ê¾ÒÀ¸¸ç, Èí¼ö¼±·®¿¡ ´ëÇÑ ¼±Çü¼ºµµ ¶Ù¾î³­ °ÍÀ¸·Î °üÃøµÇ¾ú´Ù. µû¶ó¼­ ±Ý¼Ó
¹Ú¸·À» ¾ñÀº TLD ¼±·®°è´Â ¸Å¿ì ÀÛÀº Å©±âÀÇ ±¤ÀÚºö°ú Ç¥¸é Èí¼ö¼±·®ÀÇ ÃøÁ¤¿¡ ¸Å¿ì ÀûÇÕ
ÇÑ °ÍÀ¸·Î »ç·áµÈ´Ù.

Purpose : An investigation has been carried out on the factors which affect the
response reading of thermoluminescent dosimeters (TLD-100) loaded with thin material
in high energy photon. The aim of the study was to assess the energy response of
TLD-100 to the therapeutic ranges of photon beam.
Materials and Methods : In this technique, TLD-100 (abbreviated as TLD) chips and
three different thin material (Tin, Gold, and Tissue equivalent plastic plate) which
mounted on the TLD chip were used in the clinical photon beam. The thickness of each
metal plates was 0.1 §® and TE plastic plate was 1 §® thick. These compared with the
photon energy dependence of the sensitivities of TLD (normal chip), TLD loaded with
Tin or Gold plate, for the photon energy range 6 MV to 15 MV, which was of interest
in radiotherapy.
Results : The enhancement of surface dose in the TLD with metal plate was clearly
detected. The TLD chips with a Gold plate was found to larger response by a factor of
1.83 in 10 MV photon beam with respect to normal chip. The sensitivity of TLD loaded
with Tin was less than that for normal TLD and TLD loaded with Gold. The relative
sensitivity of TLD loaded with metal has little energy dependence.
Conclusion : The good stability and linearity with respect to monitor units of TLD
loaded with metal were demonstrated by relative measurements in high energy Photon
(6¡­15 MV) beams. The TLD laminated with metals embedded system in solid water
phantom is a suitable detector for relative dose measurements in a small beam size and
surface dose.

Å°¿öµå

¿­Çü±¤¼±·®°è(TLD); ºñ±³ °¨¼ö¼º; ¿¡³ÊÁö ÀÇÁ¸¼º; TLD; Relative sensitivity; Energy dependence;

¿ø¹® ¹× ¸µÅ©¾Æ¿ô Á¤º¸

   

µîÀçÀú³Î Á¤º¸

KCI
KoreaMed
KAMS