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Table 1. Profiles of sesions observed

in
by Sallyann Bryant, Pablo Romero, Benedict Du Boulay

Table 3: RMS error observed in tested profiles Profile PID RL

in Intelligent Control of Closed-Loop Sedation in Simulated ICU Patients
by Brett L. Moore , Eric D. Sinzinger, Todd M. Quasny, Larry D. Pyeatt 2004
Cited by 1

Table 1. The first column lists observed molecular species, the next three columns list the SEST observational parameters and the last column gives observed main-beam brightness temperature (Tmb) and rms noise towards the maser A.

in Shocked molecular gas towards the supernova remnant G359.1 -- 0.5 and
by The Snake Lazendic, J. S. Lazendic, P M. Wardle, M. G. Burton, F. Yusef-zadeh, J. B. Whiteoak, A. J. Green, M. C. B. Ashley
"... In PAGE 2: ... The final data were smoothed over three channels. The observed transitions, frequencies and antenna beamsizes (FWHM) are listed in Table1 . For the 12CO, 13CO and CS transitions we obtained maps with approximately half-beam and one-beam sampling intervals at lower and higher transitions respectively.... In PAGE 2: ... A set of spectra on-source and at offsets of 20 arcsec in RA and Dec. was obtained for each of the other molecular transitions listed in Table1 , with integration times of 180s at each position. 3 RESULTS AND ANALYSIS 3.... In PAGE 4: ... Compared with the 13CO spectra, the 12CO and HCO+ spectra, and to a lesser extent the CS spectra, all show an absorption feature between 220 and 25kms21. In Table1 we list the results of a Gaussian fit to the 13CO feature, but for the other species affected by absorption we give only the maximum of the observed line profiles, which thus represent the minimum Tmb for these species. Figure 5.... ..."

Table 1. Observational Parameters. Frequency Vel. Res. Beam

in Molecular Gas in the NGC 6334 Star Formation Region
by Kathleen Kraemer James, James M. Jackson
"... In PAGE 6: ... Intensity calibration followed the chopper-wheel method in which the signal from a load at ambient temperature is compared to that from blank sky (the o position) (Ulich amp; Haas, 1976). Intensities are reported on the Tmb scale: Tmb = T A= mb ( Table1 ). A xed o position was observed for all but the CO J = 1 ! 0 observations: ; = 17h15m00s; ?35 0000000.... ..."

Table 2 Measured and simulated RMS widths for the horizontal and vertical extracted beam profiles

in On the Energy Dependence of Proton Beam Extraction With a Bent Crystal
by Arduini Elsener Fidecaro, U. Mikkelsen A, E. Weisse A, K. Winter
"... In PAGE 6: ...on, the measured and simulated r.m.s. widths for the horizontal and vertical extracted beam profiles at the three beam energies are shown in Table2 . The background in the measured profiles has been sub- tracted.... ..."

Table 2: Summary of some characteristics of the different dose profiles shown in this report. The beam and photon irradiations refer to the scaling with respect to 0.15 Gy/h, corresponding to =0. All doses are given as dose rates in units of Gy/h.

in Dose profiles in ECAL crystals for various irradiation conditions
by Mika Huhtinen Cern, Mika Huhtinen
"... In PAGE 9: ...elow 0.15 Gy/h to allow a folding of the dose rate distribution with the proper damage dependence. This makes it very difficult to estimate the differences in damage for different dose profiles. Table2 makes an attempt to compare some characteristics of the profiles, mainly the maximum, the minimum and the average dose. The observations we can make are very much the same as can be concluded from the preceding figures.... In PAGE 10: ... Thus the average dose in the crystal is not necessarily proportional to the total damage. Indeed, if we compare the average dose in Table2 for front and side irradiations, we find that they differ by a factor of 5.5.... In PAGE 10: ...MS qualification criteria indicate an average difference by a factor of 1.8, only [9]. This is a clear indication of the complicated dependence between dose rate and damage. The profiles of 120 GeV electron irradiation and LHC radiation doses look very different, but the charac- teristics collected in Table2 are surprisingly similar. In particular, the average is rather close to the LHC expectation of the maxima are fitted to agree.... In PAGE 10: ... In particular, the average is rather close to the LHC expectation of the maxima are fitted to agree. Table2 confirms the observation made from the figures that irradiations with a 400 MeV/c pion beam (FWHM 2 cm) give a rather good reproduction of the LHC dose profiles. In addition to this agreement of dose profiles, pion irradiations should be considered as complementary tests, since pions will be ideal projectiles to test possible effects of nuclear interactions and high LET tracks in the crystals.... ..."

Table 2: Optical parameters at the three beam profile detectors in the CPS-SPS transfer channel (TT2).

in Trajectory And Optical Parameters In A Non-Linear Stray Field
by Manglunki Martini Cern

Table 3 Theoretical and experimental results for wide and narrow beams with single and double thickness. Narrow Beam, h Narrow Beam, 2h Wide Beam, h Wide Beam, 2h

in Damage Detection In Simulated Aging-Aircraft Panels Using The Electro-Mechanical Impedance Technique
by Victor Giurgiutiu, Andrei Zagrai
"... In PAGE 7: ... The beam natural frequencies were identified from the E/M impedance spectrum. The results are given in Table3 , Exp. columns.... In PAGE 7: ... Free-free boundary conditions, and the associated mode shapes and frequency expressions (Inman 1996) were used during the simulations. The predicted first 6 resonances for flexural vibrations are shown in the Theory columns of Table3 . It should be noted that the errors are small, and within the range normally accepted in experimental modal analysis.... In PAGE 7: ...0 0 5 10 15 20 25 30 Frequency, kHz Re Z , O h m s Experimental Calculated Figure 16 Experimental and calculated spectra of frequencies for single thickness narrow beam. The effect of beam width is demonstrated by comparison of Narrow Beam and Wide Beam columns in Table3 . The experimental results indicate cluster of frequencies, which move to higher frequencies as the width of the beam is reduced.... In PAGE 7: ...lso influenced by the thickness, i.e., they shift to higher frequencies as the thickness is increased. This is also noticeable in Table3 , which shows that the lowest cluster appeared for single thickness wide specimen and the highest cluster for double thickness narrow beam, Another important aspect that needs to be noticed is that the first axial mode of vibrations is at 25 kHz. This explains the ~25 KHz double frequencies observed in the single- thickness beams, both narrow and wide.... ..."

Table 1. Profile Monitors

in Architecture-Aware Hierarchical Probabilistic Source Optimization 1
by N. Z. Azeemi
"... In PAGE 2: ... We add software performance monitors (SPM) to observe the behavior in the layers above the hardware. A typical list of HPMs and SPMs is shown in Table1 that we use in our extended framework. 2.... ..."

Table 2: Temporal differential expression profile observed in RNA transcription study

in unknown title
by unknown authors 2007
"... In PAGE 11: ... Down-reg- ulation dominates the former and up-regulation the latter interval. Complete results are tabulated in Table2 . On the whole, down-regulation is statistically more significant and 2.... ..."
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