NUCLEAR MAGNETIC RESONANCE NUCLEAR MAGNETIC RESONANCE
TABLE 1	(Continued)				y/tóWT s-			TABLE 1	(Continued)					
					Gyromagnetic	Resonance							Gyromagnetic	Resonance
Atomic		Natural		Quadrupole	ratio	frequency		Atomic		Natural		Quadrupole	ratio	frequency
weight/		abundance	Sensitivity	moment	(107 rad	CH TMS		weight/		abundance	Sensitivity	moment	(I07 rad	CH TMS
element	Spin	(%)	(versus °C)	(10 78 m:)	T-' sec"1)	100 MHz)		element	Spin	(%)	(versus "C)	(10 -M m:l	T-' sec')	100 MHz)
"Ca		0.145	5.27 x 10-	-0.05	-1.8001	6.729		"5Ba	1	6.59	1.83	0.18	2.6575	9.934
"Sc	i	100	1.71 x 10'	-0.22	6.4982	24.292		"7Ba	i	11.32	4.41	0.28	2.9728	11.113
«Ti	!	7.28	0.864	0.29	±1.5084	5.639		138 La	5	0.09	0.43	-0.47	3.5295	13.194
**Ti	j	5.51	1.18	0.24	±1.5080	5.638		""La	i	99.91	3.36 x 10=	0.2!	3.7787	14.126
»v		0.24	0.755	±0.21	2.6491	9.970		iiipr	i	100	1.66 x 10'	-5.9 x 10 ■	7.836	29.291
"V	Í	99.76	2.15 x 10-	-5.2 x I0";	7.0362	26.303		"'Nd	ä	12.17	2.31	-0.48	1.455	5.438
"Cr	i	9.55	0.49	±3 x 10":	-1.5120	5.652		■«Nd	7 i	8.3	0.37	-0.25	0.895	3.346
"Mn	1	100	9.94 x 102	0.55	6.6195	24.745		"7Sm	i	14.97	1.26	-0.21	1.104	4.128
!7Fe		2.19	4.2 x 10 '	—	0.8661	3.238		'"Sm	i	13.83	0.59	6 x 10 7	0.880	3.289
"Co	i	100	1.57 X 10'	0.40	6.3472	23.727	D	"'Eu	I	47.82	4.83 x 10:	1.16	6.634	24.801
<iNj		1.19	0.24	0.16	-2.3904	8.936		l3!Eu	1	52.18	45.3	2.9	2.930	10.952
s'Cu	]	69.09	3.65 x 10-	-0.211	7.0965	26.528		'"Cd	1	14.73	0.23	16	1.022	3.820
t!Cu	3	30.91	2.01 x I0:	-0.195	7.6018	28.417		l57Gd	j	15.68	0.48	2	1.277	4.775
k'Zn		4.11	0.665	0.!5	1.6737	6.257		"Tb	i	100	3.31 x I0;	1.3	6.067	22.679
«Ga	}	60.4	2.37 x 10-'	0.178	6.420	24.001		iftlQy	i	18.88	0.45	1.4	0.881	3.295
7'Ga	}	39.6	3.19 x |0:	0.112	8.158	30.497		l6'Dy	i	24.97	1.59	1.6	1.226	4.584
7'Ge	}	7.76	0.617	-0.2	-9.331	3.488		'"Ho	i	100	1.03 x 10'	2.82	5.487	20.513
"AS	j	100	1.43 x 10:	0.3	4.5804	17.123		'*'Er	i	22.94	0.66	2.83	0.773	2.890
77Se		7.58	2.98	—	5.1018	19.072		"Tm	t	100	3.21	—	-2.21	8.272
"Br	j	50.54	2.26 x 10=	0.33	6.7023	25.054		171 Yb	1 2	14.27	4.05	_	4.72	17.612
8lBr	;	49.46	2.77 x I0:	0.28	7.2246	27.007		l7'Yb	i	16.08	1.14	(-)"	1.31	4.852
8'Kr	;	11.55	1.23	0.15	-1.029	3.848		l7"Lu		—	—	—	—	—
»<Rb	i	72.15	43	0.25	2.5828	9.655		l7'Lu	i	97.41	1.56 x 10:	5.68	3.05	11.407
B7Rb	i	27.85	2.77 x I0;	0.12	8.7532	32.721		'7*Lu	7	2.59	5.14	8.1	2.10	7.872
B7Sr	i	7.02	1.07	0.36	-1.1593	4.334		|77Hf	j	18.50	0.88	4.5	0.95	4,008
"Y	i	100	0.668	—	-1.3108	4.900		l79Hf	s	13.75	0.27	5.1	-0.609	2.518
"Zr		11.23	6.04	-0.21	-2.4868	9.296		'*'Ta	l	99.988	2.04 x 10:	3	3.2073	11.990
»'Nb	1	100	2.740 x 10'	-0.2	6.5476	24.476			1 3	14.28	5.89 x 10 -	—	1.1145	4.166
"Mo	1	15.72	2.88	±0.12	1.7433	6.517		"»Re	1	37.07	2.8 x I0;	2.8	6.0255	22.525
"Mo	1	9.46	1.84	±1.1	-1.7799	6.654		,37Re	i	62.93	4.90 x 10=	2.6	6.0862	22.752
Tc	1	100	1.562 x 103''	-0.19''	6.0211	22.508		"7Os	i	1.64	1.14 x 10'	—	0.610?	2.282
*Ru	f	12.72	0.83	7.6 x 10 :	-1.2343	4,614	i	!S90s	i	16.1	2.13	o.s	2.0773	7.765
,0lRu	}	17.07	1.56	0.44	-1.3834	5.171		'"Ir	i	37.3	2.3 x 10-'	1.5	0.539	1.718
""Rh		100	0.177	—	-0.8520	3.185		"'Ir	i	62.7	5.0 x I0-2	1.4	0.391	1.871
io<Pd		22.23	1.41	0.8	-0.756	4.576			i	33.8	19.1	—	5.7412	21.462
107 Ag		51.82	0.195	—	-1.0828	4.048		"7Au	i	100	6.0 x \0-	0.58	0.357	1.729
mAg		48.18	0.276	—	-1.2448	4.654		™Hg	i	16.84	5.42	—	4.7912	17.911
'"Cd		12.75	6.93	—	-5.6714	21.201		»i Hg	i	13.22	1.08	0.5	-1.7686	6.612
'"Cd		12.26	7.6	—	-5.9328	22.178		™n	i	29.50	2.89 x 10:	—	15.3078	57.224
'"In	1	4.28	83.8	1.14	5.8493	21.866		insT1	i	70.50	7.69 x I0:	—	15.4584	57.787
"'In	i	95.72	1.89 x 10'	0.83	5.8618	21.913			i	22.6	11.8	—	5.5797	20.858
'"Sn	i	0.35	0.695	—	-8.792	32.86		;mBi	!	100	7.77 X 10;	-0.4	4.2986	16.069
"'Sn		7.61	19.54	_	-9.5319	35.632			i	—	—	—	—	—
'"Sn		8.58	25.2	—	-9.9756	37.291		23! (J	i	0.72	4.9 x 10 '	4.1	0.479	1.791
,:'Sb		57.25	5.20 x 10-	-0.53	6.4016	23.931								
	2													
l:'Sb	i	42.75	1.11 x 10;	-0.68	3.4668	12.959	I	" Most values taken from Brevard, C,			and Grager, P.	(1981). "Handbook of High Resolution Multinuclear		
l:'Te	1	0.89	0.89	_	-7.0006	26.170		NMR,"	Wiley (Interscience). New York, pp. 80-211.					
,:'Te	j	7.0	12.5		-8.4398	31.550		* Some values taken from the Bruker NMR-NQR Periodic Table: Harris, R. K.					and Mann. B. E.	(1978). "NMR
117,	I	100	5.3 x 10:	-0.79	5.3525	20.009		and the Periodic Table."		' Academic Press, London, pp. 5-7; Pople, J. A., Schneider, W. C, and Bernstein, H. J.				
"»Xe	i	26.44	31.8	—	-7.4003	27.658		(1959). '	'High-Resolution Nuclear Magnetic Resonance,			' McGraw-Hill. New York. pp. 480-485		; Harris, R. K.
»'X«	i	21.18	3.31	-0.12	2.1939	8.200		private communication						
'"Cs	{	100	2.69 x 10:	-3 x 10-'	3.5087	13.116		' Poorly known or unknown.						
								d Franklin. K. I.. lock. C I 1    Saver R			T.    anH Srhrnhiloen  ft  t  11 Qft*> 1   /  A      Chem  Knr  101 SlfR-SUIf,			
						(continues)	O							
TABLE I.   Properties of Magnetically Active Nuclides" *
Atomic weight/ element
Spin
Natural abundance
m
Sensitivity (versus l3C)
Quadrupole moment (10~:8 m2)
Gyromagnetic ratio (IO7 rad T*1 sec')
Resonance frequency CH TMS 100 MHz)
'H	4	99.985	5.68 x 10J	—	26.7510	100.0000
*H	1	0.015	8.2 x IO"3	2.73 x 10"3	4.1064	15.351
'H	i		—	—	28.5335	106.663
3He		0.00014	3.26 x 10-J	—	-20.378	76.178
6Li		7.42	3.58	-8 x IO"4	3.9366	14.716
7Li	I	92.58	1.54 x 103	-4.5 x 10":	10.3964	38.864
»Be	i	100	78.8	5.2 x 10-:	-3.759	14.052
ioB	3	19.58	22.1	7.4 x IO"2	2.8740	10.744
"B		80.42	7.54 x 10:	3.55 x IO"2	8.5794	32.072
,3C	j	1.108	1.00	—	6.7283	25.145
MN		99.63	5.69	1.6 x IO"2	1.9331	7.226
	|	0.37	2.19 x 10"2	—	-2.7116	10.137
i7o		0.037	6.11 x 10--	-2.6 x IO"2	-3.6264	13.556
	j	100	4.73 x I03	—	25.181	94.094
:;Ne	j	0.257	3.59 x 10"2	9 x IO"2	-2.1118	7.894
23Na	i	100	5.25 x 10:	0.12	7.0761	26.452
«Mg	j	10.13	1.54	0.22	-1.6375	6.122
rAl	j	100	1.17 x 103	0.149	6.9704	26.057
29Si	i	4.70	2.09	—	-5.3146	19.867
jip		100	3.77 x 10:	—	10.8289	40.481
33S	j	0.76	9.73 x 10":	-5.5 x IO"2	2.0534	7.676
"CI		75.53	20.2	-8.0 x IO"2	2.6210	9.798
37C1	j	24.47	3.8	-6.32 x IO'2	2.1817	8.156
	1	93.1	2.69	5.5 x IO"2	1.2483	4.666
	4	0.012	3.52 x 10"3	(-V	-1.552	5.801
4,K		6.88	3.28 x 10":	6.7 x IO"2	0.6851	2.561