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MC50 ½ÎÀÌŬ·ÎÆ®·Ð¿¡¼­ »ý¼ºµÇ´Â Áß¼ºÀÚ¼±ÀÇ »ý¹°ÇÐÀû Ư¼ºÀÇ Æò°¡ Evaluation of Biological Characteristics of Neutron Beam Generated from MC50 Cyclotron

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¾ö±Ù¿ë, ¹Ú¼®¿ø, ¿ìÈ«±Õ, ¹ÚÇýÁø, Çã¼ø³ç, ¿¹¼ºÁØ, À̵¿ÇÑ,
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¾ö±Ù¿ë ( Eom Keun-Yong ) 
¼­¿ï´ëÇб³ ÀÇ°ú´ëÇÐ ¹æ»ç¼±Á¾¾çÇб³½Ç

¹Ú¼®¿ø ( Park Suk-Won ) 
Áß¾Ó´ëÇб³º´¿ø
¿ìÈ«±Õ ( Wu Hong-Gyun ) 
¼­¿ï´ëÇб³ ÀÇ°ú´ëÇÐ ¹æ»ç¼±Á¾¾çÇб³½Ç
¹ÚÇýÁø ( Park Hae-Jin ) 
¼­¿ï´ëÇб³ ÀÇ°ú´ëÇÐ ¹æ»ç¼±Á¾¾çÇб³½Ç
Çã¼ø³ç ( Huh Soon-Nyung ) 
¼­¿ï´ëÇб³ ÀÇ°ú´ëÇÐ ¹æ»ç¼±Á¾¾çÇб³½Ç
¿¹¼ºÁØ ( Ye Sung-Joon ) 
¼­¿ï´ëÇб³ ÀÇ°ú´ëÇÐ ¹æ»ç¼±Á¾¾çÇб³½Ç
À̵¿ÇÑ ( Lee Dong-Han ) 
¿øÀÚ·ÂÀÇÇпø ¹æ»ç¼±Á¾¾çÇаú

Abstract

¸ñ Àû: ¿øÀÚ·ÂÀÇÇпø¿¡ ¼³Ä¡µÇ¾î ÀÖ´Â MC50 »çÀÌŬ·ÎÆ®·Ð¿¡¼­ »ý¼ºµÇ´Â Áß¼ºÀÚ¼±ÀÇ ÀÇÇÐÀû ÀÌ¿ëÀ» À§ÇÏ¿© »ý¹°ÇÐÀû Ư¼ºÀ» Æò°¡ÇÏ°íÀÚ ÇÏ¿´´Ù.

´ë»ó ¹× ¹æ¹ý: 35 MeV ¾ç¼ºÀÚ¸¦ 15 mm º£¸±·ý Ç¥Àû¿¡ ºÎµúÇô¼­ »ý¼ºµÈ Áß¼ºÀÚ¼±¿¡ ´ëÇÏ¿© ¹°¸®Àû ¹æ»ç¼±¼±·®À» ÃøÁ¤ÇÑ ÈÄ Ã¼¿Ü½ÇÇè(in-vitro)À» ÇÏ¿´´Ù. EMT-6 ¼¼Æ÷ÁÖ(cell line)¸¦ ÀÌ¿ëÇÏ¿© 0¢¦5 GyÀÇ Áß¼ºÀÚ¼±À» Á¶»ç ÈÄ »ýÁ¸ºÐȹ(surviving fraction)À» ±¸ÇÏ¿´´Ù. ¶ÇÇÑ °¨¸¶¼±ÀÇ È¿°ú¸¦ ÇÇÇϱâ À§ÇÏ¿© ³³Â÷Æó¸¦ ÇÑ ÈÄ¿¡ µ¿ÀÏ Á¶°Ç¿¡¼­ »ýÁ¸ºÐȹÀ» ±¸ÇÏ¿´´Ù. ¿¢½º¼± ½ÇÇè¿¡¼­´Â 0, 2, 5, 10, 15 Gy¸¦ Á¶»ç ÈÄ »ýÁ¸ºÐȹÀ» ÃøÁ¤ÇÏ¿´´Ù.

°á °ú: MC50ÀÇ Áß¼ºÀÚ¼±Àº Á¶»ç¾ß 26¡¿26 cm2, Àü·ù 10¥ìA, ±íÀÌ 2 cm¿¡¼­ 84%ÀÇ Áß¼ºÀÚ¿Í 16%ÀÇ °¨¸¶¼±À¸·Î ±¸¼ºµÇ¾î ÀÖ¾ú°í, ÃѼ±·®·üÀº 9.25 cGy/minÀ̾ú´Ù. ¿¢½º¼±À» ÀÌ¿ëÇÏ¿© ÃøÁ¤ÇÑ »ýÁ¸ºÐȹ°î¼±Àº ¼±ÇüÀÌÂ÷ÇÔ¼ö¸ðµ¨ (linear quadratic model)À» Àû¿ëÇÏ¿´À» ¶§ ¥á/¥âºñ´Â 0.611 (¥á=0.0204, ¥â=0.0334, R2=0.999)À̾ú´Ù. Áß¼ºÀÚ¼±¿¡ À־ »ýÁ¸ºÐȹ°î¼±Àº Àú¼±·® ¿µ¿ª¿¡¼­ ¾î±ú¿µ¿ª(shoulder area)À» °¡Áö°í ÀÖ¾ú°í, ¸ðµç ½ÇÇè¿¡¼­ ¼±ÇüÀÌÂ÷ÇÔ¼ö¸ðµ¨¿¡ Àß ¸Â¾Ò´Ù. ¥áÀÇ Æò±Õ°ªÀº -0.315 (¹üÀ§, -0.254¢¦-0.360)¿´°í, ¥â°ªÀº 0.247 (¹üÀ§, 0.220¢¦0.262)À̾ú´Ù. ³³Â÷Æó¸¦ ÇÏ¿´À» ¶§¿¡µµ »ýÁ¸ºÐȹ°î¼±¿¡¼­ ¾î±ú¿µ¿ªÀº ¾ø¾îÁöÁö ¾Ê¾Ò´Ù. Áß¼ºÀÚ¼±ÀÇ RBE (relative biological effectiveness) °ªÀº »ýÁ¸ºÐȹÀÌ 0.1ÀÏ ¶§ 2.07¢¦2.19 ¹üÀ§¿´°í, 0.01ÀÏ ¶§ 2.21¢¦2.35¿´´Ù.

°á ·Ð: MC50¿¡¼­ »ý¼ºµÈ Áß¼ºÀÚ¼±Àº »ó´ç·®ÀÇ °¨¸¶¼±À» ³»Æ÷ÇÏ°í ÀÖÀ¸¸ç ÀÌ°ÍÀÌ »ýÁ¸ºÐȹ°î¼±¿¡¼­ ¾î±ú¿µ¿ªÀÌ ³ªÅ¸³ª´Â µ¥¿¡ ±â¿©ÇÏ¿´À» °ÍÀÌ´Ù. MC50ÀÇ Áß¼ºÀÚ¼±ÀÇ RBE °ªÀº ¾à 2.2¿´´Ù.

Purpose: To evaluate biological characteristics of neutron beam generated by MC50 cyclotron located in the Korea Institute of Radiological and Medical Sciences (KIRAMS).

Materials and Methods: The neutron beams generated with 15 mm Beryllium target hit by 35 MeV proton beam was used and dosimetry data was measured before in-vitro study. We irradiated 0, 1, 2, 3, 4 and 5 Gy of neutron beam to EMT-6 cell line and surviving fraction (SF) was measured. The SF curve was also examined at the same dose when applying lead shielding to avoid gamma ray component. In the X-ray experiment, SF curve was obtained after irradiation of 0, 2, 5, 10, and 15 Gy.

Results: The neutron beams have 84% of neutron and 16% of gamma component at the depth of 2 cm with the field size of 26¡¿26 cm2, beam current 20¥ìA, and dose rate of 9.25 cGy/min. The SF curve from X-ray, when fitted to linear-quadratic (LQ) model, had 0.611 as ¥á/¥â ratio (¥á=0.0204, ¥â=0.0334, R2=0.999, respectively). The SF curve from neutron beam had shoulders at low dose area and fitted well to LQ model with the value of R2 exceeding 0.99 in all experiments. The mean value of alpha and beta were -0.315 (range, -0.254¢¦-0.360) and 0.247 (0.220¢¦0.262), respectively. The addition of lead shielding resulted in no straightening of SF curve and shoulders in low dose area still existed. The RBE of neutron beam was in range of 2.07¢¦2.19 with SF=0.1 and 2.21¢¦2.35 with SF=0.01, respectively.

Conclusion: The neutron beam from MC50 cyclotron has significant amount of gamma component and this may have contributed to form the shoulder of survival curve. The RBE of neutron beam generated by MC50 was about 2.2.

Å°¿öµå

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Cyclotron;Neutron;RBE;Raiation therapy

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KCI
KoreaMed
KAMS