V01 V1, V8, V10, V20, V86; these stars located around the cluster RGB tip are V01 classified as LPVs. They are saturated in all the HST frames and in the V01 Subaru 180s long exposures. Only the TNG and Subaru frames with texp=30s V01 were used to derive their light curves and pulsation properties. V02 this RRab is about 1mag brighter than the HB, and being at the center of V02 the cluster it is likely contaminated by companion stars which also may V02 cause the bumpy light curves from 0.2 to 0.6 in phase. V08 V1, V8, V10, V20, V86; these stars located around the cluster RGB tip are V08 classified as LPVs. They are saturated in all the HST frames and in the V08 Subaru 180s long exposures. Only the TNG and Subaru frames with texp=30s V08 were used to derive their light curves and pulsation properties. V10 V1, V8, V10, V20, V86; these stars located around the cluster RGB tip are V10 classified as LPVs. They are saturated in all the HST frames and in the V10 Subaru 180s long exposures. Only the TNG and Subaru frames with texp=30s V10 were used to derive their light curves and pulsation properties. V20 V1, V8, V10, V20, V86; these stars located around the cluster RGB tip are V20 classified as LPVs. They are saturated in all the HST frames and in the V20 Subaru 180s long exposures. Only the TNG and Subaru frames with texp=30s V20 were used to derive their light curves and pulsation properties. V27 data from the TNG set are very scattered. The Fourier analysis gives V27 several aliases which makes it difficult to define the period. The star V27 was also observed by Baade (1935ApJ....82..396B). The three sets of data V27 (this paper, Baade, and PR, Pinto & Rosini, 1977A&AS...28..427P) are not V27 phased by the same period, probably because the period changed from V27 P=0.35184-days by Baade, to P=0.34896-days by PR, to the value V27 P=0.34519-days inferred from our data. V37 there is a shift in magnitude between Subaru and TNG light curves; we used V37 both data sets to define the period, but only the Subaru data to derive V37 mean magnitudes and amplitudes. V39 double-mode RR Lyrae star with period ratio P1/P0=0.745. In Table 2, we V39 report the pulsation characteristics of the first-overtone (FO) pulsation; V39 the pulsation characteristics of the fundamental mode are P_F_=0.54621d, V39 A_V_=0.347mag, A_B_=0.454mag, and A_I_=0.305mag. V44 this star is very bright and is saturated in the HST frames and in the V44 Subaru 180s exposures; only the TNG images and the Subaru frames with V44 texp=30s could be used to derive its pulsation properties. The star has V44 P~0.9-days and rather small amplitudes. According to the position on the V44 CMD, V44 falls in the region of LPVs. V45 the star is very close to the cluster center. The Subaru data provide a V45 V amplitude larger than do the TNG data. In Table 2, we have reported the V45 visual amplitude inferred from the Subaru data; the amplitude of the TNG V45 data is A_V_>0.416mag. V46 the star is in the central part of the cluster and likely contaminated by V46 other stars. We have used only the Subaru data because these are less V46 scattered than the TNG observations. V54 the star, classified as first-overtone RR Lyrae, has small amplitudes V54 likely because it is contaminated by two companion stars. V62 the star is contaminated by a very luminous source. The Subaru data are V62 not usable and the TNG data are very scattered. V65 V65, V71, V79, V76; these stars are in the central part of the cluster. V65 There are systematic shifts among TNG, Subaru, and HST data sets of the V65 four stars likely due to crowding and blending effects. All three data V65 sets were used to estimate the periods, but only the Subaru data to V65 derive average magnitudes and amplitudes. V70 there is a shift in magnitude between TNG and Subaru data sets for the V70 star. In the present analysis, we used only the TNG data which produce a V70 smoother light curve. V71 V65, V71, V79, V76; these stars are in the central part of the cluster. V71 There are systematic shifts among TNG, Subaru, and HST data sets of the V71 four stars likely due to crowding and blending effects. All three data V71 sets were used to estimate the periods, but only the Subaru data to V71 derive average magnitudes and amplitudes. V76 V65, V71, V79, V76; these stars are in the central part of the cluster. V76 There are systematic shifts among TNG, Subaru, and HST data sets of the V76 four stars likely due to crowding and blending effects. All three data V76 sets were used to estimate the periods, but only the Subaru data to V76 derive average magnitudes and amplitudes. V79 V65, V71, V79, V76; these stars are in the central part of the cluster. V79 There are systematic shifts among TNG, Subaru, and HST data sets of the V79 four stars likely due to crowding and blending effects. All three data V79 sets were used to estimate the periods, but only the Subaru data to V79 derive average magnitudes and amplitudes. V80 the star is near a very bright source. Only the TNG data set was used since V80 it produced smoother light curves. V83 the star is in the blue straggler region and is tentatively classified as a V83 SX Phoenicis variable. However, with a period of about 0.14-days it V83 significantly deviates from the SX Phe period-luminosity (PL) relation V83 (see Figure 13). V86 V1, V8, V10, V20, V86; these stars located around the cluster RGB tip are V86 classified as LPVs. They are saturated in all the HST frames and in the V86 Subaru 180s long exposures. Only the TNG and Subaru frames with texp=30s V86 were used to derive their light curves and pulsation properties. V87 binary system. In Table 2, we list the most probable period inferred for V87 the star by the Lomb periodogram since it gives less scatter than the V87 period inferred from the Fourier analysis (P=0.184716-days, A_V_=1.199mag, V87 A_B_=0.166mag, and A_V_>0.265mag). V89 the star has very small amplitudes for a c-type RR Lyrae. It lies very V89 close to the edge of the frames and this may partially explain the V89 anomalous amplitudes.