ライフサイエンスコーパス: rad

1 el from an average 2.2 rad (0.022 Gy) to 1.0 rad (0.010 Gy) (P < .001).

2 -low Faraday rotation measure regime (<1,000 rad m(-2)).

3 ylactic cranial radiation to a dose of 3,000 rad.

4 er a broad range of frequencies (0.1-30, 000 rad/s), LTM provides a unique ability to noninvasively q

5 horacic radiation therapy consisted of 4,000 rad to the tumor and mediastinum with a 1,000-rad boost.

6 amster somatic hybrid cell panel and a 5,000 rad whole-genome radiation hybrid (WGRH) panel.

7 rel (millicurie) injected was 90 Gy/g (9,000 rad/g), of which 64% was from conversion electrons, 16%

8 ad to the tumor and mediastinum with a 1,000-rad boost.

9 This study shows that the 10,000-rad panel is appropriate for the generation of a high-re

10 A 10,000-rad radiation hybrid (RH) cell panel of the rhesus macaq

11 igh-resolution RH map of SSC12 on the 12,000-rad IMNpRH2 panel using CarthaGene software.

12 Analysis of the 5,000-rad horse x hamster radiation hybrid panel produced a ma

13 12 short tandem repeat markers on the 5,000-rad horse x hamster whole-genome radiation hybrid panel

14 ences were added to the Illinois-Texas 5,000-rad RH (RH, radiation hybrid) map.

15 The high-resolution Illinois-Texas 5,000-rad RH and comparative maps will facilitate identificati

16 A high-resolution SSC12 RH12,000-rad map will be useful in fine-mapping QTL and as a scaf

17 cle-average vorticity (male: 0.006 +/- 0.001 rad-m(2)/ml-s; female: 0.011 +/- 0.002 rad/s; p=0.001) w

18 0.001 rad-m(2)/ml-s; female: 0.011 +/- 0.002 rad/s; p=0.001) were all significantly higher in the LV

19 tolic vorticity index (male: 0.008 +/- 0.005 rad-m(2)/ml-s; female: 0.014 +/- 0.007 rad-m(2)/ml-s; p=

20 tolic vorticity index (male: 0.007 +/- 0.006 rad-m(2)/ml-s; female: 0.014 +/- 0.010 rad-m(2)/ml-s; p=

21 0.005 rad-m(2)/ml-s; female: 0.014 +/- 0.007 rad-m(2)/ml-s; p=0.007), peak diastolic vorticity index

22 d 0.0020 mGy/MBq (0.0086, 0.0006, and 0.0074 rad/mCi) for the ovaries, testes, and red marrow, respec

23 his wire with an error of approximately 0.01 rad, whereas typical energy scales are of the order of 1

24 0.006 rad-m(2)/ml-s; female: 0.014 +/- 0.010 rad-m(2)/ml-s; p=0.015), and cycle-average vorticity (ma

25 The whole-body dose is 0.0111 rad/mCi, resulting in a 0.622 rad exposure with a maximu

26 ains an AoA mean of 0.08 radians (SD = 0.014 rad), a TDoA mean of 0.020 s (SD = 0.003 s), and a FoA m

27 (0.0295 rad/mCi) and 0.00709 mGy/MBq (0.0262 rad/mCi), respectively.

28 rrow and spleen were 0.00797 mGy/MBq (0.0295 rad/mCi) and 0.00709 mGy/MBq (0.0262 rad/mCi), respectiv

29 Ba2+-sensitive admittance was 3.09 +/- 0.03 rad at 10 Hz and 3.00 +/- 0.17 rad at 30 Hz.

30 the lipid tail rotation (D(rot_tail) = -0.04 rad(2)/ns) is slower then the head group rotation (D(rot

31 ps and an out of plane rate of Dtheta = 0.05 rad(2)/ps.

32 to the pancreas, and 0.0186 mGy/MBq (0.0688 rad/mCi) to the uterus.

33 ffusively at an in plane rate of Dphi = 0.07 rad(2)/ps and an out of plane rate of Dtheta = 0.05 rad(

34 ver (mean, 24.78 rad/mCi; range, 15.02-37.07 rad/mCi), with red marrow estimates on the order of 3.32

35 /mCi) to the kidneys, 0.0197 mGy/MBq (0.0728 rad/mCi) to the pancreas, and 0.0186 mGy/MBq (0.0688 rad

36 he critical organ receiving a dose of 0.0886 rad/mCi.

37 lags peak tidal extension by approximately 1 rad, suggestive of resonance.

38 typical energy scales are of the order of 1 rad.

39 nd 67Cu-BAT-2IT-1A3 were 586 and 1269 rad (1 rad = 0.01 Gy), respectively.

40 of the laser trap at frequencies less than 1 rad/s, indicating that at least locally, the gels behave

41 ived a radiation dose of 0.028 mGy/MBq (0.10 rad/mCi).

42 within the range of frequency from 0.1 to 10 rad/s, with a maxima viscoelastic layer at alkaline pH (

43 lated (>/=75.6 Gy to 90 Gy) EBRT (1 Gy = 100 rad).

44 The low-frequency (< or = 100 rad s-1) impedance of skin was much more significantly a

45 strain over a frequency range of 0.1 to 100 rad/sec.

46 The dose was 0.027 mGy/MBq (0.101 rad/mCi) to the kidneys, 0.0197 mGy/MBq (0.0728 rad/mCi)

47 64Cu- and 67Cu-BAT-2IT-1A3 were 586 and 1269 rad (1 rad = 0.01 Gy), respectively.

48 lungs, with a dose of 0.0393 mGy/MBq (0.1455 rad/mCi).

49 from 0.0002 to 0.0393 mGy/MBq (0.0006-0.1455 rad/mCi).

50 ation-associated LD(50) being reduced by 150 rad.

51 Tumor dosimetry ranged from 39 to 167 rad/mCi of 90Y (442-1887 rad/ dose).

52 3.09 +/- 0.03 rad at 10 Hz and 3.00 +/- 0.17 rad at 30 Hz.

53 h received an average of 0.046 mGy/MBq (0.17 rads/mCi, range 0.14-0.22 rad/mCi).

54 (0.59 rem) and a lung dose of 21.8 mGy (2.18 rad) in young, healthy subjects.

55 nged from 39 to 167 rad/mCi of 90Y (442-1887 rad/ dose).

56 ere the lower large intestine (1.43 +/- 0.19 rad/mCi) and upper large intestine (1.20 +/- 0.38 rad/mC

57 fferent frequencies ranging from omega = 0.2 rad/s to 6.9 rad/s.

58 yed and unenhanced (-1.6+/-0.8 to -2.3+/-1.2 rad/s).

59 sing the radiation level from an average 2.2 rad (0.022 Gy) to 1.0 rad (0.010 Gy) (P < .001).

60 hen the head group rotation (D(rot_hg) = 2.2 rad(2)/ns), which is slower than the overall in plane (D

61 ower than the overall in plane (D(rot) = 3.2 rad(2)/ns) for the lipid molecule.

62 t across the film is an odd multiple of pi/2 rad.

63 the nano-bunched beam can be O(10(21)A/m(2)/rad(2)) orders of magnitude higher than current XFEL bea

64 .046 mGy/MBq (0.17 rads/mCi, range 0.14-0.22 rad/mCi).

65 h received an average of 0.062 mGy/MBq (0.23 rad/mCi, range 0.08-0.30 rad/mCi), followed by the kidne

66 ctions were quantified to be as fast as 3.25 rad s(-1) and as large as 0.5 A, respectively.

67 ,w)|, over a range of frequencies (w = 1-250 rad/second) in excised tumors within minutes with a spat

68 .65 +/- 0.32 rad at 10 Hz and -2.79 +/- 0.26 rad at 30 Hz.

69 ts (n=51) underwent a single, rapid (117-266 rad/s) head rotation in the sagittal (n=13), coronal (n=

70 dose of 0.15 +/- 0.08 mGy/MBq (0.57 +/- 0.28 rad/mCi).

71 ovement velocities tested (ie, 4.71 and 6.28 rad/s).

72 ge decreases with a value of 7.5 mGy/MBq (28 rad/mCi) for a newborn.

73 tients demonstrated that |G*(x,y,w)| (w = 2n rad/second) closely corresponds with histological featur

74 ntwisting velocity, -2.0+/-0.7 to -5.6+/-2.3 rad/s) that was associated with an increase in IVPG (1.4

75 .3 and 2.2 +/- 0.5 mGy/MBq (2.4, 3.8 and 8.3 rad/mCi), respectively.

76 0.062 mGy/MBq (0.23 rad/mCi, range 0.08-0.30 rad/mCi), followed by the kidneys (0.051 mGy/MBq), liver

77 l mortality included radiation dose >/= 3000 rad ( >/= 30 Gy; supra-diaphragm: HR, 3.8; 95% CI, 1.1-1

78 Irradiation (3000 rads) of the i.v. donor splenocytes combined with RIB 5/

79 digrees informative for XLPRA, and on a 3000-rad canine-hamster radiation hybrid (RH) panel.

80 ap and 37 were positioned on the Roslin 3000-rad radiation hybrid (RH) map, with 20 assignments share

81 ve admittance in GP cells was -2.65 +/- 0.32 rad at 10 Hz and -2.79 +/- 0.26 rad at 30 Hz.

82 .07 mSv/MBq (0.64 +/- 0.18 and 0.55 +/- 0.32 rad/mCi) for females and males, respectively.

83 th red marrow estimates on the order of 3.32 rad/mCi (range, 1.24-5.55) of 90Y.

84 y bladder wall dose to 0.0885 mGy/MBq (0.327 rad/mCi) or 0.128 mGy/MBq (0.473 rad/mCi), respectively,

85 ich received an estimated 0.11 mGy/MBq (0.37 rad/mCi).

86 Ci) and upper large intestine (1.20 +/- 0.38 rad/mCi).

87 ceiving the highest dose, 0.11 mGy/MBq (0.39 rad/mCi).

88 ies with a statistical uncertainty of 10(-4) rad.

89 /s and a Coriolis parameter of 1.05 x 10(-4) rad/s (latitude of ~46 ) would give a transitional scale

90 s) but converge at high frequencies (> 10(4) rad/s).

91 g. the 'no-load' angular velocity is ca. 400 rad/s anticlockwise at 4 mM ATP.

92 was transferred to irradiated ACI rats (400 rad) with either purified T cells (4-10 x 10[7]) or seru

93 myeloma, SCID mice were irradiated with 400 rads and mice were injected either with 10(6) ARH-77 cel

94 ch received an average of 0.12 mGy/MBq (0.43 rad/mCi) (range, 0.098-0.15 mGy/MBq).

95 One species with omega(0) = 0.45 rad/ns and low eta is attributed to a trigonal planar Cd

96 /MBq (0.327 rad/mCi) or 0.128 mGy/MBq (0.473 rad/mCi), respectively, and the effective dose to 0.0149

97 e in-plane diffusive reorientations with 1.5 rad(2)/s rotational diffusivity, a value that compares w

98 ers of magnitude at low frequencies (0.5-1.5 rad/s) but converge at high frequencies (> 10(4) rad/s).

99 was 16 mGy (1.6 rad) (range, 4-45 mGy [4-4.5 rad]).

100 ccurately, giving a tumor dose of 81 +/- 7.5 rad/mCi.

101 n, it would have taken 22.7 mCi to deliver 5 rad to the liver.

102 injected dose at 56 mCi using the limit of 5 rads to a critical organ per study per year.

103 After sublethal radiation injury (500 rad), the infusion of purified CD4(+) T cells enhances h

104 Sublethal irradiation (500 rad) of mice prior to tumor inoculation abrogated the IL

105 immunosensitizing sublethal irradiation (500 rad) of the host before adoptive therapy.

106 Mice rendered pancytopenic with 500 rads and 1.2 mg of carboplatin had a nadir platelet coun

107 developed by testing DNA samples from a 5000 rad whole genome RH panel.

108 A second-generation 5000 rad radiation hybrid (RH) map of the cattle genome was c

109 as obtained using the recently produced 5000(rad) horse x hamster hybrid panel.

110 We recently constructed a 5000-rad cattle whole-genome radiation hybrid panel with the

111 ere mapped primarily by genotyping on a 5000-rad horse x hamster radiation hybrid panel, of which 28

112 A 5000-rad whole genome radiation hybrid panel is described for

113 enerated in this study and typed to our 5000-rad horse x hamster whole genome RH panel.

114 as the urinary bladder at 0.14 mGy/MBq (0.51 rad/mCi).

115 mCi]), followed by liver (0.14 mGy/MBq [0.52 rad/mCi]); the effective dose is 0.022 mSv/MBq (0.083 re

116 estion (ie, 12.48+/-0.95 versus 11.11+/-0.53 rad/s; P<0.05).

117 g, max rotational head acceleration was 5388 rad/s(2), max linear head velocity was 3.8 m/s and max r

118 ssion occurs is approximately 100 g and 5500 rad/s/s.

119 ministered activity was 0.150 mGy/MBq (0.556 rad/mCi) with the realistic void schedule used in our st

120 and large intestines (161.26 muGy/MBq [0.597 rad/mCi] and 184.59 muGy/MBq [0.683 rad/mCi]).

121 average fetal radiation dose was 16 mGy (1.6 rad) (range, 4-45 mGy [4-4.5 rad]).

122 /s and max rotational head velocity was 21.6 rad/s.

123 (66 mCi) to give the same dose rate of 43.6 rad/h in the lungs at 48 h.

124 rils is more mechanically rigid (517 Pa at 6 rad/s) than the gel composed of twisted fibrils (367 Pa

125 gel composed of twisted fibrils (367 Pa at 6 rad/s).

126 ls with peak reorientation speeds of up to 6 rad/s and returning to random after 5 min without stimul

127 Although the addition of 600 rad of total body irradiation delayed tumor growth, furt

128 e kidney capsule of diabetic irradiated (600 rads), naive C57BL/6 recipients (mean survival time = 48

129 est (0.39) with an angular frequency of 0.62 rad/s.

130 dose is 0.0111 rad/mCi, resulting in a 0.622 rad exposure with a maximum single injection dose.

131 blood (131)I was 0.34 (range, 0.1 6 to 0.63) rad/mCi (0.09 mGy/MBq; range, 0.04 to 0.17 mGy/ MBq).

132 I(rad) and MAT in seconds (s): MAT=64-63xCFI(rad) ( r(2)=0.229; P<0.0001).

133 q [0.597 rad/mCi] and 184.59 muGy/MBq [0.683 rad/mCi]).

134 rgan is gallbladder wall (0.19 mGy/MBq [0.69 rad/mCi]), followed by liver (0.14 mGy/MBq [0.52 rad/mCi

135 f 2 less than the value of 0.45 mGy/MBq (1.7 rad/mCi) previously accepted.

136 nit of administered 131I was 1.0 Gy/GBq (3.7 rad/mCi) for patients with NHL whether in MTD or LD tria

137 rying random signal with a velocity of 10(7) rad/s.

138 , and gallbladder wall, 0.193 mGy/MBq (0.716 rad/mCi).

139 treatment absorbed dose limit of 75 cGy (75 rad), the administered 131I activity ranged from 2.1 to

140 lculated in this study of 0.21 mGy/MBq (0.77 rad/mCi) is approximately a factor of 2 less than the va

141 ses were delivered to the liver (mean, 24.78 rad/mCi; range, 15.02-37.07 rad/mCi), with red marrow es

142 ved the highest dose (229.50 muGy/MBq [0.849 rad/mCi]), followed by the small and large intestines (1

143 ion, we achieve modulation depths up to 4.85 rad with 80 mW of applied microwave power at 2.31 GHz in

144 encies ranging from omega = 0.2 rad/s to 6.9 rad/s.

145 to amplitudes of approximately 1.5 x 10(-9) rad at the lowest frequency normal mode and the sensitiv

146 tion rotation angle (1sigma) of 5.6 x 10(-9) rad/ Hz, which corresponds to an absorption sensitivity

147 the target organ or tissue of 19.4 mGy (1.93 rad).

148 d, MHC class II +/+ mice and irradiated (950 rads) MHC class II -/- recipients.

149 e urinary bladder wall, 0.258 mGy/MBq (0.955 rad/mCi), and gallbladder wall, 0.193 mGy/MBq (0.716 rad

150 We propose that atl-1 and rad-5/clk-2 respond to single-stranded DNA generated by

151 Phenotypic comparison of Cebrc-2 and rad-51 mutants also revealed a role for CeBRC-2 in an er

152 c and cytological comparisons of Cebrc-2 and rad-51 mutants revealed fundamental phenotypic differenc

153 n DNA repair defects observed in Cebrc-2 and rad-51 mutants, and define mechanistic roles for CeBRC-2

154 that atl-1 (Caenorhabditis elegans ATR) and rad-5/clk-2 prevent mitotic catastrophe, function in the

155 e stress activates ataxia telangiectasia and rad-3-related (ATR) and Chk1 checkpoint kinases that inh

156 ate of bone tissue sustains radial camellae (rad) in a condition similar to Alamosaurus and Saltasaur

157 CFI(rad) was equal to 0.802+/-0.150 (95% CI, 0.783-0.820).

158 11, and patients with abnormal MAT had a CFI(rad) of 0.648+/-0.224 ( P<0.0001).

159 The group with normal MAT had a CFI(rad) of 0.830+/-0.111, and patients with abnormal MAT ha

160 e was an inverse linear relation between CFI(rad) and MAT in seconds (s): MAT=64-63xCFI(rad) ( r(2)=0

161 for CFI during radial artery occlusion (CFI(rad)) and CFI during radial plus ulnar artery occlusion.

162 ndard prescribed absorbed dose of 7,000 cGy (rad) to the thyroid therefore was reduced by over 50% wi

163 hyperthyroidism, with a standard 7,000-cGy (rad) thyroid absorbed dose generally resulting in an inc

164 tal blood absorbed dose of less than 10 cGy (rad).

165 dental blood absorbed dose of up to 150 cGy (rad) could result.

166 ATDs, from 11.3 +/- 6.5 to 4.9 +/- 2.8 cGy (rad) (P < 0.001).

167 s exceeding the MTA safety limit of 200 cGy (rads) to the blood or bone marrow in many patients with

168 raction between hus1+ and another checkpoint rad gene, rad1+.

169 uires rad3+ and each of the other checkpoint rad genes.

170 combination machinery and the six checkpoint rad gene products plus the Cdsl kinase.

171 UV at a level equivalent to some checkpoint rad mutants.

172 9 acts in a process involving the checkpoint rad genes and that the rhp9 mutant is phenotypically ver

173 x fission yeast genes, termed the checkpoint rad genes, which are essential for both the S-M and DNA

174 process which is defective in the checkpoint rad mutants and which involves hus5 .

175 s complex is dependent on a third checkpoint rad gene, rad9+, suggesting that these three proteins ma

176 Whereas checkpoint rad mutants fail to arrest division in response to DNA d

177 The waveform average curvature (rad/mum) was also conserved as the cilium grew.

178 to a less severe defect seen in rad9 delta, rad 17 delta, and rad24 delta.

179 ned to be 7.62 +/- 0.15 (standard deviation) rad/ms.

180 in PCMH[Y384F] which produced PchF[Y384F]FAD(rad) x PchC, the mutant enzyme containing the flavin rad

181 n of unassociated PchC(ox) by PchF[Y384F]FAD(rad) x PchC.

182 Fl(rad)(*-) undergoes a homogeneous proton transfer reactio

183 )H(-) (E(0)(f) = -1.05 V vs Fc/Fc(+)) and Fl(rad)(*2-) (E(0)(f) = -1.62 V vs Fc/Fc(+)), respectively.

184 y one electron to form the radical anion (Fl(rad)(*-)) at E(0)(f) = -1.22 V versus Fc/Fc(+) (E(0)(f)

185 n rates, the homogeneous reaction between Fl(rad)(*-) and Fl(ox) begins to be outrun, which leads to

186 ciated with the one-electron reduction of Fl(rad)(*-) to form Fl(red)(2-) (E(0)(f) = -1.98 V vs Fc/Fc

187 the starting material (Fl(ox)) to produce Fl(rad)H(*) and Fl(ox)(-), which are both able to undergo f

188 1-Dy through 4-Dy and the magnitude of J(Gd-rad) for the corresponding gadolinium derivatives that p

189 gnets 1-Dy through 4-Dy, where stronger J(Gd-rad) for the corresponding Gd(3+) compounds is associate

190 he magnetic exchange coupling constant, J(Gd-rad), for the gadolinium compounds in this series to be

191 omolog of the S. pombe rad1 checkpoint gene, rad-5, and him-7-block both DNA damage-induced apoptosis

192 k markers previously mapped on the IMpRH7000-rad SSC12 and porcine genetic maps.

193 r, relocalization appears more frequently in rad-5 mutants, suggesting that RAD-5 plays a role in rep

194 ce tumor-to-nontumor ratios and may increase rad doses to tumor more selectively than directly labele

195 From k(rad) and k(rad) + k(nonrad), we compute a theoretical photoluminesc

196 pressure-dependent radiative conductivity, k(rad), from these data is 2-5 times lower than previously

197 seen in LHCs-with radiative rate constant (k(rad)) exceeding that of a single linker.

198 From k(rad) and k(rad) + k(nonrad), we compute a theoretical ph

199 Radiative recombination ( k(rad)) is calculated through oscillator strengths using S

200 As confirmed by these studies strong Ln-rad coupling is achieved, with 1 exhibiting slow magneti

201 The blood absorbed dose (cGy/37 MBq [rad/mCi] administered) was reduced from 2.54 +/- 0.91 (m

202 nstant alpha to be (-1 +/- 0.34) x 10(-10) N/rad(2); and 3) the ciliary base may be an essential regu

203 calculated to be (4.6 +/- 0.62) x 10(-12) N/rad and nonlinear spring constant alpha to be (-1 +/- 0.

204 exoskeletons (rotational stiffness: 0-250 Nm rad(-1)) in one training and two testing days.

205 ere maximized (4.2%) at a stiffness of 50 Nm rad(-1).

206 orque: G(stall) ~ 3 k(B)T/rad (or 0.01 nN.nm/rad).

207 ich a torsional spring constant of ~23 pN.nm/rad(2) is estimated on average for all S1 types, similar

208 s of kinks and cross-links of ~100-200 pN.nm/rad.

209 alternative repair pathway in the absence of rad-51 and independent of nonhomologous end joining (NHE

210 rror-prone DSB repair pathway independent of rad-51 and non-homologous end joining, raising the possi

211 ng HR but can also function independently of rad-51 in DSB repair processes.

212 to DNA damage and can do so independently of rad-51.

213 We have previously shown that loss of rad-23 improves locomotor deficits in TDP-43 C. elegans

214 ion forks by RPA-1 and functions upstream of rad-5/clk-2 in the S-phase checkpoint.

215 tient-specific mean 90Y dose (cGy/37 MBq, or rad/mCi) was 0.53 (0.32-0.78) to whole body, 3.75 (0.63-

216 cell cycle events and coordinates with other rad/hus checkpoint gene products in responding to radiat

217 -nature radical dearomatases P450(rad1)-P450(rad)(5) facilitated asymmetric dearomatization of a broa

218 fluorescence to long-lived phosphorescence (rad-M1BNM, tau(RTP) =232 ms) is observed.

219 1 +/- 183 pN.mum(2) and ks = 39.3 +/- 6.0 pN/rad under the same conditions.

220 al dynein interactions ( approximately 35 pN/rad) to interdoublet sliding resistance in these immobil

221 ibutions of the N-DRCs ( approximately 40 pN/rad) and residual dynein interactions ( approximately 35

222 0 +/- 280 pNmum(2) and ks = 79.6 +/- 10.5 pN/rad, respectively.

223 7 +/- 184 pN.mum(2) and ks = 43.3 +/- 7.7 pN/rad.

224 e identification of homologs of the S. pombe rad checkpoint genes from mammals, arthropods, and nemat

225 National Institutes of Health's RADx-rad initiative, National Science Foundation, Virginia G

226 Silencing requires rad-2, gei-17, and the polh-1 translesion DNA polymerase

227 over the second-generation EST SSC12 RH7000-rad map of 103 ESTs and 15 framework markers covering ap

228 The protein products of several rad checkpoint genes of Schizosaccharomyces pombe (rad1+

229 iciency eDf25, is allelic to rfs-1, the sole rad-51 paralog group member in C. elegans.

230 net (Philips) with SSH MRCP 3DHR and SSHMRCP rad protocol.

231 l), and the stall torque: G(stall) ~ 3 k(B)T/rad (or 0.01 nN.nm/rad).

232 t that mutations in the smk-1 gene cause the rad-2 phenotype.

233 with defects in the DNA damage aspect of the rad checkpoint control pathway had an increased frequenc

234 We recently found that the rad-2 mutation alleviates this checkpoint silent DNA dam

235 course, known to radiology residents as the "rad-path" course, was not a casualty of the BRAC, the Am

236 a single dose of 16 or 18 Gy (to convert to rad, multiply by 100) given to the involved vertebral le

237 Unlike rad-51 mutants, Cebrc-2 mutants also accumulate RPA-1 at

238 gnated mec1-srf for synthetic lethality with rad-fifty-two) simultaneously cause two types of phenoty

239 In this study, a fission yeast rad mutant (slp1-362) was genetically investigated.