... 8.20 7.76 M/M _ 0.57 0.54 1.22 0.50 0.54 0.85 1.17 1.12 0.61 1.29 0.53 0.45 0.94 0.70 0.52 0.65 0.51 0.66 1.29 0.51 0.82 0.65 0 ...

... k 2 H = h 2 DA et ­ G NA exp RT 4 m RT * m (57) We can further simplify the analysis by defining the partial derivative 0 G m ...

... N. Teleman: Combinatorial Thom­Hirzebruch Characteristic Classes. IHES/M/57, pp. 1­25, ґ Inst. Hautes Etudes Sci., Bures-sur-Yvette, Paris, 1999. ...

... 51 Peg . 5.5 . G5 V . 22 h 57 m .5 . +20 o 46' . 0".074 . 1995-2003 . ...

... model QQQ tsound Q Q QQ Q Q Q Q Q QQQ Q Q QQ (i) concool 0, (ii) rapid cooling t Q Q Q 4) QQQQ dynamical timescale 26) Q QQ Q Q Q QQ QQ 57 10 M Q Q 1996 QQQ Q z 1.4 UV Q Q Q IMF Q Q Q QQ Q Salpeter (1955) Q Kroupa (2007) 0.5M Q5 Q QQ QQQQ QQ Q QQ QQ QQQ ...

... 55. " " , u(M ) M 0 . 56. " " , u(M ) M . 57. " " , b u(M ) M 0 . 58. , {(x , y ) : x 2 + y 2 1} . 59. 60. 61. , {(x , y ) : x 2 + y 2 > 1} . ...

... We see from the figure that the predicted mass distribution function is defined only in the mass interval 0.57­0.7 M . ...

... 02:56 - 05:09 М . 02:49 - 05:10 В . (Армстронг) . 03:15 - 04:57 M . 03:11 - 05:03 В . (Олдрин) . 2:32+ . ...

... 00015 CALL PTICR0(AK,U,X1,X2,Y1,Y2,N,M) 00016 H=1.E-10 00017 DO 57 I=1,N 00018 X=X1+HX*(I-1.) ... 2/0.03))/0.955040800- -0.0521309113 00020 57 CONTINUE 00021 CALL PTICR3(U,Z0,U0,N,M) 00022 PRINT 501,(Z0(II),II=1,N) 00023 501 ...

... 56 D. Basmadjian, Can. J. Chem., 1960, 38, 141. 57 D. M. Ruthven and R. L. Derrah, J. Chem. Soc., Faraday Trans. 1, 1975, 71, 2031. ...