267 research outputs found
NASA/GE quiet engine C acoustic test results
The acoustic investigation and evaluation of the C propulsion turbofan engine are discussed. The engine was built as a part of the Quiet Engine Program. The objectives of the program are as follows: (1) to determine the noise levels produced turbofan bypass engines, (2) to demonstrate the technology and innovations which will reduce the production and radiation of noise in turbofan engines, and (3) to acquire experimental acoustic and aerodynamic data for high bypass turbofan engines to provide a better understanding of noise production mechanisms. The goals of the program called for a turbofan engine 15 to 20 PNdB quieter than currently available engines in the same thrust class
Acoustic testing of a 1.5 pressure ratio, low tip speed fan (QEP fan B scale model)
A scale model (0.484 scale factor) of a single stage fan designed for a 1.5 pressure ratio and 1160 ft/sec tip speed was tested to determine its noise characteristics. The fan had 26 blades and 60 outlet guide vanes, with vanes spaced two rotor blade aerodynamic chords from the blades. The effects of speed, exhaust nozzle area and fan frame acoustic treatment on the scale model's noise characteristics were investigated
Clustering of Photometric Luminous Red Galaxies II: Cosmological Implications from the Baryon Acoustic Scale
A new determination of the sound horizon scale in angular coordinates is
presented. It makes use of ~ 0.6 x 10^6 Luminous Red Galaxies, selected from
the Sloan Digital Sky Survey imaging data, with photometric redshifts. The
analysis covers a redshift interval that goes from z=0.5 to z=0.6. We find
evidence of the Baryon Acoustic Oscillations (BAO) signal at the ~ 2.3 sigma
confidence level, with a value of theta_{BAO} (z=0.55) = (3.90 \pm 0.38)
degrees, including systematic errors. To our understanding, this is the first
direct measurement of the angular BAO scale in the galaxy distribution, and it
is in agreement with previous BAO measurements. We also show how radial
determinations of the BAO scale can break the degeneracy in the measurement of
cosmological parameters when they are combined with BAO angular measurements.
The result is also in good agreement with the WMAP7 best-fit cosmology. We
obtain a value of w_0 = -1.03 \pm 0.16 for the equation of state parameter of
the dark energy, Omega_M = 0.26 \pm 0.04 for the matter density, when the other
parameters are fixed. We have also tested the sensitivity of current BAO
measurements to a time varying dark energy equation of state, finding w_a =
0.06 \pm 0.22 if we fix all the other parameters to the WMAP7 best-fit
cosmology.Comment: 7 pages, 7 figures, Accepted for publication to MNRA
Acoustic testing of a 1.5 pressure ratio low tip speed fan with a serrated rotor (QEP fan B scale model)
A scale model of the bypass flow region of a 1.5 pressure ratio, single stage, low tip speed fan was tested with a serrated rotor leading edge to determine its effects on noise generation. The serrated rotor was produced by cutting teeth into the leading edge of the nominal rotor blades. The effects of speed and exhaust nozzle area on the scale models noise characteristics were investigated with both the nominal rotor and serrated rotor. Acoustic results indicate the serrations reduced front quadrant PNL's at takeoff power. In particular, the 200 foot (61.0 m) sideline noise was reduced from 3 to 4 PNdb at 40 deg for nominal and large nozzle operation. However, the rear quadrant maximum sideline PNL's were increased 1.5 to 3 PNdb at approach thust and up to 2 PNdb at takeoff thust with these serrated rotor blades. The configuration with the serrated rotor produced the lowest maximum 200 foot (61.0 m) sideline PNL for any given thust when the large nozzle (116% of design area) was employed
Π€ΠΠ ΠΠΠ ΠΠΠΠΠΠ ΠΠ ΠΠ‘ΠΠΠ‘ΠΠΠΠ’ΠΠΠ¬ΠΠ«Π₯ Π ΠΠΠΠ¦ΠΠ Π£Π§ΠΠ©ΠΠ₯Π‘Π― Π ΠΠΠΠΠ‘ΠΠΠΠ‘Π’Π ΠΠ’ Π’ΠΠΠ ΠΠ‘ΠΠ₯ΠΠΠΠΠΠ’ΠΠ’ΠΠΠΠΠ Π ΠΠΠ£ΠΠ―Π¦ΠΠ
The purpose of the students (12 to 15 years old) examination was to identify the integrative criteria of assessing the nature of the functional relationships between the parameters of the psychosocial and physiological adaptation of students, depending on age, individual-typological peculiarities of vegetative regulation, personal potential at different stages of school education.The study of the characteristics of vegetative regulation of the cardiovascular system was made with a help of an automatic cardiac-rhythm programs. The research of psychophysiological parameters was fulfiled using an automatic complex. The measurement of the speed of simple visual-motor reaction (PSMR), reaction to a moving object (WFD), the level of functional mobility of nervous processes (WFP) and health brain (DDM) were made before. Features psychosocial adaptation was analyzed using 8-color Luscher test.All examinee were divided into three groups on the basis of the statistical characteristics of the cardiac rhythm by the tone source autonomic tone: βvagotoniaβ (with a predominance of parasympathetic sistems), βsomatotonicβ (with domination of the sympatholytic effects), βatonicβ (balanced type of vegetative nervous system).Based on the analysis of psychodynamic, neurodynamic and vegetative functions showed that students with initial vagotonies tone are characterized by high levels of situational and personal anxiety, low psychosocial adaptation, decreased activity of neurodynamic functions and psychodynamic processes in the learning dynamics, whereas the individuals with dominance of sympatotonics type regulation have high level of neurodynamic processes, psychosocial adaptation, against the background of significant stress mechanisms of vegetative regulation.Students with initial vegetative tone demonstrate a sufficient level of psychosocial adaptation, activity psychodynamic and neuromotor processes, accompanied by the preservation of the functionality of the body according to the parameters myocardial-hemodynamic homeostasis.It is established that the formation process of psychosocial and physiological adaptation and disadaptation of students is largely determined by the type of vegetative (autonomic) tone, degree of stress, behaviour strategies in stressful situations.Π¦Π΅Π»ΡΡ ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½Π½ΠΎΠ³ΠΎ ΡΡΠ΅Π΄ΠΈ ΡΡΠ°ΡΠΈΡ
ΡΡ Π² Π²ΠΎΠ·ΡΠ°ΡΡΠ΅ ΠΎΡ 12 Π΄ΠΎ 15 Π»Π΅Ρ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΡΠ²ΠΈΠ»ΠΎΡΡ Π²ΡΡΠ²Π»Π΅Π½ΠΈΠ΅ ΠΈΠ½ΡΠ΅Π³ΡΠ°ΡΠΈΠ²Π½ΡΡ
ΠΊΡΠΈΡΠ΅ΡΠΈΠ΅Π² ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»Π΅ΠΉ, ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡΡΠΈΡ
ΠΎΡΠ΅Π½ΠΈΡΡ Ρ
Π°ΡΠ°ΠΊΡΠ΅Ρ ΡΡΠ½ΠΊΡΠΈΠΎΠ½Π°Π»ΡΠ½ΡΡ
Π²Π·Π°ΠΈΠΌΠΎΡΠ²ΡΠ·Π΅ΠΉ ΠΌΠ΅ΠΆΠ΄Ρ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠ°ΠΌΠΈ ΠΏΡΠΈΡ
ΠΎΡΠΎΡΠΈΠ°Π»ΡΠ½ΠΎΠΉ ΠΈ ΡΠΈΠ·ΠΈΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΎΠΉ Π°Π΄Π°ΠΏΡΠ°ΡΠΈΠΈ ΡΡΠ°ΡΠΈΡ
ΡΡ Π² Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΎΡ Π²ΠΎΠ·ΡΠ°ΡΡΠ½ΡΡ
, ΠΈΠ½Π΄ΠΈΠ²ΠΈΠ΄ΡΠ°Π»ΡΠ½ΠΎ-ΡΠΈΠΏΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎΡΡΠ΅ΠΉ Π²Π΅Π³Π΅ΡΠ°ΡΠΈΠ²Π½ΠΎΠΉ ΡΠ΅Π³ΡΠ»ΡΡΠΈΠΈ, Π»ΠΈΡΠ½ΠΎΡΡΠ½ΠΎΠ³ΠΎ ΠΏΠΎΡΠ΅Π½ΡΠΈΠ°Π»Π° Π½Π° ΡΠ°Π·Π»ΠΈΡΠ½ΡΡ
ΡΡΠ°ΠΏΠ°Ρ
ΠΎΠ±ΡΡΠ΅Π½ΠΈΡ ΡΠΊΠΎΠ»ΡΠ½ΠΈΠΊΠΎΠ².ΠΠ·ΡΡΠ΅Π½ΠΈΠ΅ ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎΡΡΠ΅ΠΉ Π²Π΅Π³Π΅ΡΠ°ΡΠΈΠ²Π½ΠΎΠΉ ΡΠ΅Π³ΡΠ»ΡΡΠΈΠΈ ΡΠ΅ΡΠ΄Π΅ΡΠ½ΠΎ-ΡΠΎΡΡΠ΄ΠΈΡΡΠΎΠΉ ΡΠΈΡΡΠ΅ΠΌΡ ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΎΡΡ ΠΏΠΎ ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»ΡΠΌ Π°Π²ΡΠΎΠΌΠ°ΡΠΈΠ·ΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠΉ ΠΊΠ°ΡΠ΄ΠΈΠΎΡΠΈΡΠΌΠΎΠ³ΡΠ°ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΏΡΠΎΠ³ΡΠ°ΠΌΠΌΡ. ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ ΠΏΡΠΈΡ
ΠΎΡΠΈΠ·ΠΈΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»Π΅ΠΉ ΠΎΡΡΡΠ΅ΡΡΠ²Π»ΡΠ»ΠΎΡΡ ΠΏΡΠΈ ΠΏΠΎΠΌΠΎΡΠΈ Π°Π²ΡΠΎΠΌΠ°ΡΠΈΠ·ΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠ°, ΡΠ°ΠΊΠΆΠ΅ Π±ΡΠ»ΠΎ ΠΏΡΠΎΠΈΠ·Π²Π΅Π΄Π΅Π½ΠΎ ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΠ΅ ΡΠΊΠΎΡΠΎΡΡΠΈ ΠΏΡΠΎΡΡΠΎΠΉ Π·ΡΠΈΡΠ΅Π»ΡΠ½ΠΎ-ΠΌΠΎΡΠΎΡΠ½ΠΎΠΉ ΡΠ΅Π°ΠΊΡΠΈΠΈ, ΡΠ΅Π°ΠΊΡΠΈΠΈ Π½Π° Π΄Π²ΠΈΠΆΡΡΠΈΠΉΡΡ ΠΎΠ±ΡΠ΅ΠΊΡ, ΡΡΠΎΠ²Π½Ρ ΡΡΠ½ΠΊΡΠΈΠΎΠ½Π°Π»ΡΠ½ΠΎΠΉ ΠΏΠΎΠ΄Π²ΠΈΠΆΠ½ΠΎΡΡΠΈ Π½Π΅ΡΠ²Π½ΡΡ
ΠΏΡΠΎΡΠ΅ΡΡΠΎΠ² ΠΈ ΡΠ°Π±ΠΎΡΠΎΡΠΏΠΎΡΠΎΠ±Π½ΠΎΡΡΠΈ Π³ΠΎΠ»ΠΎΠ²Π½ΠΎΠ³ΠΎ ΠΌΠΎΠ·Π³Π°. ΠΡΠΎΠ±Π΅Π½Π½ΠΎΡΡΠΈ ΠΏΡΠΈΡ
ΠΎΡΠΎΡΠΈΠ°Π»ΡΠ½ΠΎΠΉ Π°Π΄Π°ΠΏΡΠ°ΡΠΈΠΈ Π°Π½Π°Π»ΠΈΠ·ΠΈΡΠΎΠ²Π°Π»ΠΈΡΡ ΠΏΡΠΈ ΠΏΠΎΠΌΠΎΡΠΈ Π²ΠΎΡΡΠΌΠΈΡΠ²Π΅ΡΠΎΠ²ΠΎΠ³ΠΎ ΡΠ΅ΡΡΠ° ΠΡΡΠ΅ΡΠ°.ΠΡΠ΅ ΠΎΠ±ΡΠ»Π΅Π΄ΡΠ΅ΠΌΡΠ΅ Π»ΠΈΡΠ° Π½Π° ΠΎΡΠ½ΠΎΠ²Π°Π½ΠΈΠΈ ΡΡΠ°ΡΠΈΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊ ΡΠ΅ΡΠ΄Π΅ΡΠ½ΠΎΠ³ΠΎ ΡΠΈΡΠΌΠ° Π±ΡΠ»ΠΈ ΡΠ°Π·Π΄Π΅Π»Π΅Π½Ρ Π½Π° ΡΡΠΈ Π³ΡΡΠΏΠΏΡ ΠΏΠΎ ΡΠΎΠ½Ρ ΠΈΡΡ
ΠΎΠ΄Π½ΠΎΠ³ΠΎ Π²Π΅Π³Π΅ΡΠ°ΡΠΈΠ²Π½ΠΎΠ³ΠΎ ΡΠΎΠ½ΡΡΠ°: Β«Π²Π°Π³ΠΎΡΠΎΠ½ΠΈΠΊΠΎΠ²Β» (Ρ ΠΏΡΠ΅ΠΎΠ±Π»Π°Π΄Π°Π½ΠΈΠ΅ΠΌ ΠΏΠ°ΡΠ°ΡΠΈΠΌΠΏΠ°ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ Π³ΠΎΡΠΎΠ²Π½ΠΎΡΡΠΈ), Β«ΡΠΈΠΌΠΏΠ°ΡΠΎΡΠΎΠ½ΠΈΠΊΠΎΠ²Β» (Ρ Π΄ΠΎΠΌΠΈΠ½ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΡΠΈΠΌΠΏΠ°ΡΠΎΠ»ΠΈΡΠΈΡΠ΅ΡΠΊΠΈΡ
Π²ΠΎΠ·Π΄Π΅ΠΉΡΡΠ²ΠΈΠΉ), Β«ΡΠΉΡΠΎΠ½ΠΈΠΊΠΎΠ²Β» (ΡΠ±Π°Π»Π°Π½ΡΠΈΡΠΎΠ²Π°Π½Π½ΡΠΉ ΡΠΈΠΏ Π²Π΅Π³Π΅ΡΠ°ΡΠΈΠ²Π½ΠΎΠΉ Π½Π΅ΡΠ²Π½ΠΎΠΉ ΡΠΈΡΡΠ΅ΠΌΡ).ΠΠ° ΠΎΡΠ½ΠΎΠ²Π°Π½ΠΈΠΈ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΠΏΡΠΈΡ
ΠΎΠ΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
, Π½Π΅ΠΉΡΠΎΠ΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΈ Π²Π΅Π³Π΅ΡΠ°ΡΠΈΠ²Π½ΡΡ
ΡΡΠ½ΠΊΡΠΈΠΉ ΠΏΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ ΡΡΠ°ΡΠΈΠ΅ΡΡ Ρ ΠΈΡΡ
ΠΎΠ΄Π½ΡΠΌ Π²Π°Π³ΠΎΡΠΎΠ½ΠΈΡΠ΅ΡΠΊΠΈΠΌ ΡΠΎΠ½ΡΡΠΎΠΌ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΠ·ΡΡΡΡΡ Π²ΡΡΠΎΠΊΠΈΠΌ ΡΡΠΎΠ²Π½Π΅ΠΌ ΡΠΈΡΡΠ°ΡΠΈΠ²Π½ΠΎΠΉ ΠΈ Π»ΠΈΡΠ½ΠΎΡΡΠ½ΠΎΠΉ ΡΡΠ΅Π²ΠΎΠΆΠ½ΠΎΡΡΠΈ, Π½ΠΈΠ·ΠΊΠΎΠΉ ΠΏΡΠΈΡ
ΠΎΡΠΎΡΠΈΠ°Π»ΡΠ½ΠΎΠΉ Π°Π΄Π°ΠΏΡΠ°ΡΠΈΠ΅ΠΉ, ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΠ΅ΠΌ Π°ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ Π½Π΅ΠΉΡΠΎΠ΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΡΠ½ΠΊΡΠΈΠΉ ΠΈ ΠΏΡΠΈΡ
ΠΎΠ΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΡΠΎΡΠ΅ΡΡΠΎΠ² Π² Π΄ΠΈΠ½Π°ΠΌΠΈΠΊΠ΅ ΠΎΠ±ΡΡΠ΅Π½ΠΈΡ, ΡΠΎΠ³Π΄Π° ΠΊΠ°ΠΊ Ρ Π»ΠΈΡ Ρ Π΄ΠΎΠΌΠΈΠ½ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΡΠΈΠΌΠΏΠ°ΡΠΎΡΠΎΠ½ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΠΈΠΏΠ° ΡΠ΅Π³ΡΠ»ΡΡΠΈΠΈ ΠΎΡΠΌΠ΅ΡΠ°Π΅ΡΡΡ Π²ΡΡΠΎΠΊΠΈΠΉ ΡΡΠΎΠ²Π΅Π½Ρ Π½Π΅ΠΉΡΠΎΠ΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΡΠΎΡΠ΅ΡΡΠΎΠ², ΠΏΡΠΈΡ
ΠΎΡΠΎΡΠΈΠ°Π»ΡΠ½ΠΎΠΉ Π°Π΄Π°ΠΏΡΠ°ΡΠΈΠΈ Π½Π° ΡΠΎΠ½Π΅ Π²ΡΡΠ°ΠΆΠ΅Π½Π½ΠΎΠ³ΠΎ Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΡ ΠΌΠ΅Ρ
Π°Π½ΠΈΠ·ΠΌΠΎΠ² Π²Π΅Π³Π΅ΡΠ°ΡΠΈΠ²Π½ΠΎΠΉ ΡΠ΅Π³ΡΠ»ΡΡΠΈΠΈ ΡΠΉΡΠΎΠ½ΠΈΡΠ΅ΡΠΊΠΈΡ
.Π¨ΠΊΠΎΠ»ΡΠ½ΠΈΠΊΠΈ Ρ ΠΈΡΡ
ΠΎΠ΄Π½ΡΠΌ Π²Π΅Π³Π΅ΡΠ°ΡΠΈΠ²Π½ΡΠΌ ΡΠΎΠ½ΡΡΠΎΠΌ Π΄Π΅ΠΌΠΎΠ½ΡΡΡΠΈΡΡΡΡ Π΄ΠΎΡΡΠ°ΡΠΎΡΠ½ΡΠΉ ΡΡΠΎΠ²Π΅Π½Ρ ΠΏΡΠΈΡ
ΠΎΡΠΎΡΠΈΠ°Π»ΡΠ½ΠΎΠΉ Π°Π΄Π°ΠΏΡΠ°ΡΠΈΠΈ, Π°ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ ΠΏΡΠΈΡ
ΠΎΠ΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΈ Π½Π΅ΠΉΡΠΎΠΌΠΎΡΠΎΡΠ½ΡΡ
ΠΏΡΠΎΡΠ΅ΡΡΠΎΠ², ΡΠΎΠΏΡΠΎΠ²ΠΎΠΆΠ΄Π°ΡΡΠΈΡ
ΡΡ ΡΠΎΡ
ΡΠ°Π½Π΅Π½ΠΈΠ΅ΠΌ ΡΡΠ½ΠΊΡΠΈΠΎΠ½Π°Π»ΡΠ½ΡΡ
Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡΠ΅ΠΉ ΠΎΡΠ³Π°Π½ΠΈΠ·ΠΌΠ°, ΡΡΠ΄Ρ ΠΏΠΎ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠ°ΠΌ ΠΌΠΈΠΎΠΊΠ°ΡΠ΄ΠΈΠ°Π»ΡΠ½ΠΎ-Π³Π΅ΠΌΠΎΠ΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ Π³ΠΎΠΌΠ΅ΠΎΡΡΠ°Π·Π°
Very large scale correlations in the galaxy distribution
We characterize galaxy correlations in the Sloan Digital Sky Survey by
measuring several moments of galaxy counts in spheres. We firstly find that the
average counts grows as a power-law function of the distance with an exponent
D= 2.1+- 0.05 for r in [0.5,20] Mpc/h and D = 2.8+-0.05 for r in [30,150]
Mpc/h. In order to estimate the systematic errors in these measurements we
consider the counts variance finding that it shows systematic finite size
effects which depend on the samples sizes. We clarify, by making specific
tests, that these are due to galaxy long-range correlations extending up to the
largest scales of the sample. The analysis of mock galaxy catalogs, generated
from cosmological N-body simulations of the standard LCDM model, shows that for
r<20 Mpc/h the counts exponent is D~2.0, weakly dependent on galaxy luminosity,
while D=3 at larger scales. In addition, contrary to the case of the observed
galaxy samples, no systematic finite size effects in the counts variance are
found at large scales, a result that agrees with the absence of large scale,
r~100 Mpc/h, correlations in the mock catalogs. We thus conclude that the
observed galaxy distribution is characterized by correlations, fluctuations and
hence structures, which are larger, both in amplitude and in spatial extension,
than those predicted by the standard model LCDM of galaxy formation.Comment: 6 pages, 7 figures to be published in Europhysics Letter
Clustering of photometric luminous red galaxies I : Growth of Structure and Baryon Acoustic Feature
The possibility of measuring redshift space (RSD) distortions using
photometric data have been recently highlighted. This effect complements and
significantly alters the detectability of baryon acoustic oscillations (BAO) in
photometric surveys. In this paper we present measurements of the angular
correlation function of luminous red galaxies (LRGs) in the photometric catalog
of the final data release (DR7) of the Sloan Digital Sky Survey II (SDSS). The
sample compromise ~ 1.5 x 10^6 LRGs distributed in 0.45 < z < 0.65, with a
characteristic photometric error of ~ 0.05. Our measured correlation centered
at z=0.55 is in very good agreement with predictions from standard LCDM in a
broad range of angular scales, . We find that the
growth of structure can indeed be robustly measured, with errors matching
expectations. The velocity growth rate is recovered as when no prior is imposed on the growth factor and the background geometry
follows a LCDM model with WMAP7+SNIa priors. This is compatible with the
corresponding General Relativity (GR) prediction for our
fiducial cosmology. If we adopt a parametrization such that , with in GR, and combine our
measurement with the corresponding ones from spectroscopic LRGs at lower
redshifts we obtain . In addition we find evidence for
the presence of the baryon acoustic feature matching the amplitude, location
and shape of LCDM predictions. The photometric BAO feature is detected with 98
% confidence level at z=0.55.Comment: 16 pages, 19 figures, minor changes to text to match accepted version
by MNRA
A Strategy to Measure the Dark Energy Equation of State using the HII galaxy Hubble Relation & X-ray AGN Clustering: Preliminary Results
We explore the possibility of setting stringent constraints to the Dark
Energy equation of state using alternative cosmic tracers like: (a) the Hubble
relation using HII galaxies, which can be observed at much higher redshifts
(z~3.5) than those currently traced by SNIa samples, and (b) the large-scale
structure using the clustering of X-ray selected AGN,which have a redshift
distribution peaking at z~1.
We use extensive Monte-Carlo simulations to define the optimal strategy for
the recovery of the dark-energy equation of state using the high redshift (z~2)
Hubble relation, but accounting also for the effects of gravitational lensing,
which for such high redshifts can significantly affect the derived cosmological
constraints. Based on a "Figure of Merit" analysis, we provide estimates for
the number of 2<z<3.5 tracers needed to reduce the cosmological solution space,
presently provided by the Constitution SNIa set, by a desired factor. We find
that it is much more efficient to increase the number of tracers than to reduce
their individual uncertainties.
Finally, we propose a framework to put constraints on the dark energy
equation of state by using the joint likelihood of the X-ray AGN clustering and
of the Hubble relation cosmological analyses. A preliminary joint analysis
using the X-ray AGN clustering of the 2XMM survey and the Hubble relation of
the Constitution SNIa set provide: Omega_m= 0.31+-0.01 and w=-1.06+-0.05. We
also find that the joint SNIa-2XMM analysis provides significantly more
stringent cosmological constraints, increasing the Figure of Merit by a factor
~2, with respect to that of the joint SNIa-BAO analysis.Comment: MNRAS in press, 12 colour figure
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