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An tV/^-like Integrin Receptor on Rat Aortic Smooth Muscle Cells
Both the original sample (Lanes 4 and 7) and the 3A3 (Lanes 5 and 8) and anti-hamster ft 32. Tomaselll KJ, Damsky CH, Reichardt LF. Purification and
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JSTOR: The Application of Runge-Kutta Schemes to Singular Initial
Hence, for m = 3' h4a2(4- 3a3)MY"(t~) + O(h3/(j + 1)). .840-10'4 .894.10-4 1/16 .122-10'3 .123.10'3 .576.10'5 .687.10'5 1/32 .153-10'4 .153.10'4
Phys. Rev. D 62, 124007 (2000): Hobbs and Dunsby - Dynamical
Point Values (w,U,V,W) Eigenvalues (l1,2,3,4) D1 (0,0,12 caE2 @ 32 kE22 89 #, const! whosecorresponding wavelength is losc52A65 lEC5 2A65 F 2pH E 4 3A3
Phys. Rev. C 68, 014901 (2003): Kapusta and Shovkovy - Thermal
014901-4 sense that grNN5grpp , a result that holds rather well nu-merically. 5 3A3 K1 2 2 5 3A3K_ 1 0 2 29 f 1 2 5A29 f~1 4 3A3 a1 0 4 3A3 a1 2 4 3A3
(IUCr) Microabsorption of X-rays in Planar Powder Samples in the
Ps(a) = #bocva[ l - 3a/2 + 3a3 (32) - 3a2(1 + a) exp (- 1/a)], 4. Microabsorption factor P as a function of the scattering angle for different values of
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