ORCHESTRATION, INSTRUMENTAL EFFECT, AND STRUCTURE

2018 ◽  
pp. 259-279
Keyword(s):  
2008 ◽  
Vol 15 (6) ◽  
pp. 987-997 ◽  
Author(s):  
E. I. Nikolopoulos ◽  
A. Kruger ◽  
W. F. Krajewski ◽  
C. R. Williams ◽  
K. S. Gage

Abstract. The authors present results of a comparative analysis of rainfall data from several ground-based instruments. The instruments include two vertically pointing Doppler radars, S-band and X-band, an optical disdrometer, and a tipping-bucket rain gauge. All instruments were collocated at the Iowa City Municipal Airport in Iowa City, Iowa, for a period of several months. The authors used the rainfall data derived from the four instruments to first study the temporal variability and scaling characteristics of rainfall and subsequently assess the instrumental effects on these derived properties. The results revealed obvious correspondence between the ground and remote sensors, which indicates the significance of the instrumental effect on the derived properties.


1972 ◽  
Vol 44 ◽  
pp. 188-189
Author(s):  
D. Alloin ◽  
Y. Andrillat ◽  
S. Souffrin

Many people have attacked the problem of synthesizing the stellar population of the galaxies. We have performed such a synthesis, by using only the intensities of absorption lines in the nuclei of galaxies. It is then possible to obtain a synthesized continuous spectrum even if there are several possible solutions for the stellar composition, and the computed continuum does not vary much with the assumed model of stellar population.The method is to fit the equivalent widths of the absorption lines using different stellar compositions. In order to avoid any instrumental effect, we have observed different lines and bands from 3500 to 8500 å in stars of various well-known stellar types and luminosity classes, under the same conditions as the galaxies.We have applied this method to some ‘ordinary’ nuclei and to some Seyfert ones. As an example, we show the results for M81 and for NGC 1068.


2015 ◽  
Vol 9 (1) ◽  
pp. 0-0
Author(s):  
Белых ◽  
E. Belykh ◽  
Несмеянов ◽  
A. Nesmeyanov ◽  
Борисова ◽  
...  

The article demonstrates the importance of the application of new biomedical technologies in the correction of somatoform disorders in athletes. In observation were 86 athletes playing sports. Comprehensive clinical, psychological and instrumental examination showed that 11, 3% of them have some somatic pathology, but the complaint didn’t match up to this pathology, she had overdone character. Moreover, in this group in 36.4% of cases, there are previous histories of acute infectious diseases. The athletes were divided into two equal groups (main and control) by 43 people. In the main group, the athletes were treated orally with shungite in the form of tablets, in the control group - the psycho-pharmacotherapy. The same clinical and instrumental effect was observed in both groups. In the control group the undesirable effect of reducing muscle tone, drowsiness was detected. This allowed the authors to consider that it is expedient to use shungite for the correction of sym-tomatics in athletes with somatoform disorders.


1979 ◽  
Vol 89 ◽  
pp. 239-240
Author(s):  
D. C. Williams

The NPL instrument to correct for angular refraction in geodesy measures the small dispersion between images of red (633 nm) and blue (442 nm) laser sources formed by a telescope. It uses a rotating chopper disc in association with an optical compensator plate and a phase null meter. The instrument and some early field tests have been described in detail elsewhere (Williams, D.C., 1978).Absolute tests of the prototype have recently been made over a 4 km suburban range at an average height of 30 m. The apparent elevation of the red laser was observed with a T3 theodolite and corrected for refraction, the laser and theodolite being referred to local bench marks with a known height difference determined by spirit levelling.On an occasion in late May 1978, the effects of turbulence were particularly small. The refraction-corrected theodolite readings then agreed with the expected value to within one sexagesimal second. Other results obtained during the preceding two months indicate that increasing turbulence causes the dispersion angle to appear too large, the greatest error observed being about 3 seconds of refraction. It is thought that most of the turbulence was due to effluent from chimneys, and that the apparent error may be due to an instrumental effect which has not yet been identified.The performance of the instrument has also been evaluated on a 20 km range near Uppsala during the present Symposium, by kind invitation of Prof. E. Tengström. The principal difference from the 4 km range was that the intensity scintillations of the red and blue signals were no longer correlated when the refraction was large. Independent compensation of red and blue signals for this effect should enable good results to be obtained over this distance.The author wishes to acknowledge the help of S-G. Mårtensson and S. Eklund (University of Uppsala) and A.J. Griffiths (NPL) in performing the tests.


2018 ◽  
Vol 863 (2) ◽  
pp. 195 ◽  
Author(s):  
Taozhi Yang ◽  
A. Esamdin ◽  
Fangfang Song ◽  
Hubiao Niu ◽  
Guojie Feng ◽  
...  

2020 ◽  
Vol 500 (2) ◽  
pp. 2264-2277 ◽  
Author(s):  
Ian Hothi ◽  
Emma Chapman ◽  
Jonathan R Pritchard ◽  
F G Mertens ◽  
L V E Koopmans ◽  
...  

ABSTRACT We compare various foreground removal techniques that are being utilized to remove bright foregrounds in various experiments aiming to detect the redshifted 21 cm signal of neutral hydrogen from the epoch of reionization. In this work, we test the performance of removal techniques (FastICA, GMCA, and GPR) on 10 nights of LOFAR data and investigate the possibility of recovering the latest upper limit on the 21 cm signal. Interestingly, we find that GMCA and FastICA reproduce the most recent 2σ upper limit of $\Delta ^2_{21} \lt $ (73)2 mK2 at k = 0.075 hcMpc−1, which resulted from the application of GPR. We also find that FastICA and GMCA begin to deviate from the noise-limit at k-scales larger than ∼0.1 hcMpc−1. We then replicate the data via simulations to see the source of FastICA and GMCA’s limitations, by testing them against various instrumental effects. We find that no single instrumental effect, such as primary beam effects or mode-mixing, can explain the poorer recovery by FastICA and GMCA at larger k-scales. We then test scale-independence of FastICA and GMCA, and find that lower k-scales can be modelled by a smaller number of independent components. For larger scales (k ≳ 0.1 hcMpc−1), more independent components are needed to fit the foregrounds. We conclude that, the current usage of GPR by the LOFAR collaboration is the appropriate removal technique. It is both robust and less prone to overfitting, with future improvements to GPR’s fitting optimization to yield deeper limits.


Sign in / Sign up

Export Citation Format

Share Document