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Dependence of the GRAPES-3 EAS particle density and trigger rate on atmospheric pressure and temperature Meeran Zuberi (on behalf of GRAPES-3 Collaboration) PoS(ICRC2017)302 ICRC 2017 July 13, 2017 Meeran Zuberi (TIFR) Atmospheric Effects on


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SLIDE 1

Dependence of the GRAPES-3 EAS particle density and trigger rate on atmospheric pressure and temperature

Meeran Zuberi

(on behalf of GRAPES-3 Collaboration) PoS(ICRC2017)302 ICRC 2017

July 13, 2017

Meeran Zuberi (TIFR) Atmospheric Effects on GRAPES-3 July 13, 2017 1 / 22

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SLIDE 2

Outline

1

Introduction

2

Atmospheric Effects on Particle Density

3

Atmospheric Effects on Trigger Rate

4

Summary

Meeran Zuberi (TIFR) Atmospheric Effects on GRAPES-3 July 13, 2017 2 / 22

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SLIDE 3

GRAPES-3 EAS Array

Located at Ooty, India (11.4◦ N, 76.7◦ E and 2.2 km m.s.l.) 400 plastic scintillation detectors (1 m2 each) covers an area of 25,000 m2 3712 proportional counters form a tracking muon telescope of area 560 m2

Meeran Zuberi (TIFR) Atmospheric Effects on GRAPES-3 July 13, 2017 3 / 22

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SLIDE 4

GRAPES-3 Shower Trigger

Two level trigger system : Level 0 : A three line coincidence used to generate this trigger. Level 1 : Minimum 10 detectors should trigger out of all detectors. Trigger Rate : 42 Hz (3.6 million EAS/day) Energy Range : 10 TeV-10 PeV

Meeran Zuberi (TIFR) Atmospheric Effects on GRAPES-3 July 13, 2017 4 / 22

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SLIDE 5

Motivation

The scintillation detectors measure particle densities and relative arrival times of secondaries. These informations are used to reconstruct the shower size, core location and arrival direction. The periodic variations in both particle density and trigger rate were

  • bserved due to atmospheric effects.

These corrections are important for more accurate measurement of shower parameters.

Meeran Zuberi (TIFR) Atmospheric Effects on GRAPES-3 July 13, 2017 5 / 22

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SLIDE 6

Atmospheric Parameters

The secondary cosmic ray flux can be influenced by the atmospheric parameters such as:

1

Atmospheric Pressure

2

Temperature

At Ooty, pressure (12 hrs) and temperature (24 hrs) display periodic behavior.

Meeran Zuberi (TIFR) Atmospheric Effects on GRAPES-3 July 13, 2017 6 / 22

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SLIDE 7

Atmospheric Effect on Particle Density

Year 2014 EAS data was used for this study. Total particles passing through each detector was obtained on hourly basis.

Time (hours) 50 100 150

(%)

UC

I/I) ∆ (

20 − 10 − 10

  • Det. 286

Particle density variation from 1 Jan 2014 to 7 Jan 2014

Meeran Zuberi (TIFR) Atmospheric Effects on GRAPES-3 July 13, 2017 7 / 22

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SLIDE 8

Fast Fourier Transform (FFT)

Cycles/Day

1 2 3 4 5

Amplitude

5 10 15 20 25

  • Det. 286

Power spectrum of particle density

Meeran Zuberi (TIFR) Atmospheric Effects on GRAPES-3 July 13, 2017 8 / 22

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SLIDE 9

Filter

W(f) ≡      1, if |f − fc| ≤ ∆f sin π

2 |f −fc| ∆f ,

if ∆f < |f − fc| ≤ 2∆f 0, if |f − fc| < 2∆f

Meeran Zuberi (TIFR) Atmospheric Effects on GRAPES-3 July 13, 2017 9 / 22

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SLIDE 10

Fast Fourier Transform (FFT)

Temperature Dependence of Particle Density

Cycles/Day

1 2 3 4 5

Amplitude

0.5 1 1.5

Power spectrum of temperature

Cycles/Day

1 2 3 4 5

Amplitude

5 10 15 20 25

  • Det. 286

Power spectrum of particle density

Meeran Zuberi (TIFR) Atmospheric Effects on GRAPES-3 July 13, 2017 10 / 22

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SLIDE 11

Fast Fourier Transform (FFT)

Temperature Dependence of Particle Density

Cycles/Day

1 2 3 4 5

Amplitude

0.5 1 1.5

Power spectrum of temperature

Cycles/Day

1 2 3 4 5

Amplitude

5 10 15 20 25

  • Det. 286

Power spectrum of particle density

Meeran Zuberi (TIFR) Atmospheric Effects on GRAPES-3 July 13, 2017 10 / 22

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SLIDE 12

Fast Fourier Transform (FFT)

The Inverse FFT was obtained by using filter on 1 cycle/day. The particle density was found to have lag with the temperature data.

10 20 30 40 50 Particle density (%) 8 − 6 − 4 − 2 − 2 4 6 8 Hours 10 20 30 40 50 C)

  • T (

∆ 6 − 4 − 2 − 2 4 6

Particle Density Temperature

  • Det. 286

Meeran Zuberi (TIFR) Atmospheric Effects on GRAPES-3 July 13, 2017 11 / 22

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SLIDE 13

Fast Fourier Transform (FFT)

The temperature data was shifted by ±3 hours in the interval of 5 min w.r.t. particle density data. Lag for each detector was calculated at maximum correlation coefficient.

Lag (min)

50 100 150 200

Correlation Coeff

0.96 − 0.94 − 0.92 − 0.9 − 0.88 − 0.86 −

  • Det. 286

Lag of ∼80 min. at -0.96

Meeran Zuberi (TIFR) Atmospheric Effects on GRAPES-3 July 13, 2017 12 / 22

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SLIDE 14

Fast Fourier Transform (FFT)

Temperature Coefficient Distribution For All Detectors

)

T

β Temperature Coefficient ( 2.5 − 2 − 1.5 − 1 − 0.5 − 0.5 1 No of Detectors 10 20 30 40 50 60 70

Mean -0.65

RMS 0.24

Mean = (-0.65 ± 0.01)%/◦C

Meeran Zuberi (TIFR) Atmospheric Effects on GRAPES-3 July 13, 2017 13 / 22

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SLIDE 15

Fast Fourier Transform (FFT)

Temperature Corrected Particle Density

Hours

50 100 150

(%)

TC

I/I) ∆ (

20 − 10 − 10

  • Det. 286

Time Variation

Cycles/Day

1 2 3 4 5

Amplitude

2 4 6 8 10

  • Det. 286

Power Spectrum

Meeran Zuberi (TIFR) Atmospheric Effects on GRAPES-3 July 13, 2017 14 / 22

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SLIDE 16

Fast Fourier Transform (FFT)

Pressure Dependence of Particle Density

Cycles/Day

1 2 3 4 5

Amplitude

0.2 0.4 0.6 0.8 1 1.2

Power Spectrum of Pressure

Cycles/Day

1 2 3 4 5

Amplitude

2 4 6 8 10

  • Det. 286

Power Spectrum of Particle Density

Meeran Zuberi (TIFR) Atmospheric Effects on GRAPES-3 July 13, 2017 15 / 22

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SLIDE 17

Fast Fourier Transform (FFT)

Pressure Dependence of Particle Density

Cycles/Day

1 2 3 4 5

Amplitude

0.2 0.4 0.6 0.8 1 1.2

Power Spectrum of Pressure

Cycles/Day

1 2 3 4 5

Amplitude

2 4 6 8 10

  • Det. 286

Power Spectrum of Particle Density

Meeran Zuberi (TIFR) Atmospheric Effects on GRAPES-3 July 13, 2017 15 / 22

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SLIDE 18

Fast Fourier Transform (FFT)

Pressure Coefficient Distribution For All Detectors

)

P

β Pressure Coefficient (

1.4 − 1.2 − 1 − 0.8 − 0.6 − 0.4 − 0.2 −

No of Detectors

20 40 60 80 100 120 140 160

Mean -0.71 RMS

0.11

Mean = (-0.710 ± 0.001)%/hPa

Meeran Zuberi (TIFR) Atmospheric Effects on GRAPES-3 July 13, 2017 16 / 22

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SLIDE 19

After Correction of Atmospheric Effects

We have performed the FFT on temperature and pressure corrected particle density data. Temperature and Pressure Corrected Particle Density

Cycles/Day

1 2 3 4 5

Amplitude

5 10 15 20

  • Det. 286

Power Spectrum

Meeran Zuberi (TIFR) Atmospheric Effects on GRAPES-3 July 13, 2017 17 / 22

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SLIDE 20

After Correction of Atmospheric Effects

50 100 150

(%)

UC

I/I) ∆ (

20 − 10 − 10

D# 286

(a)

Time (Hours) 50 100 150

(%)

PTC

I/I) ∆ (

20 − 10 − 10

(b)

Particle density (%) variation before (a) and after correction (b) of atmospheric effects

Meeran Zuberi (TIFR) Atmospheric Effects on GRAPES-3 July 13, 2017 18 / 22

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SLIDE 21

Atmospheric Effects on Trigger Rate

Trigger rate also shows the similar variations.

Hours 50 100 150 Trigger Rate (Hz) 30 30.5 31 31.5 32 32.5

(a)

Cycles/Day 1 2 3 4 5 Trigger Rate Amplitude (Hz) 100 200 300 400 500 600

(b)

Trigger rate variation (a) and its power spectrum (b)

Meeran Zuberi (TIFR) Atmospheric Effects on GRAPES-3 July 13, 2017 19 / 22

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SLIDE 22

Atmospheric Effects on Trigger Rate

C)

  • T (

10 − 8 − 6 − 4 − 2 − 2 4 6 8 10

I/I) % ∆ (

2.5 − 2 − 1.5 − 1 − 0.5 − 0.5 1 1.5 2 2.5

C

  • 0.002 ) % /

± ( -0.392

Trigger Rate Vs Temperature

P (hPa) ∆

2 − 1.5 − 1 − 0.5 − 0.5 1 1.5 2

I/I) % ∆ (

1 − 0.8 − 0.6 − 0.4 − 0.2 − 0.2 0.4 0.6 0.8 1

0.008 ) % /hPa ± ( -0.597

Trigger Rate Vs Pressure

Meeran Zuberi (TIFR) Atmospheric Effects on GRAPES-3 July 13, 2017 20 / 22

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SLIDE 23

Summary

The measured particle density shows the anti-correlation with atmospheric pressure and temperature. We have corrected the atmospheric effects from particle density by using FFT method. The similar effects have been observed in trigger rate for which temperature and pressure coefficient values have been determined by using FFT method. The correction of atmospheric effects from particle density can be used to calculate the hourly detector’s gain, which will improve the accuracy in the measurement of shower parameters.

Meeran Zuberi (TIFR) Atmospheric Effects on GRAPES-3 July 13, 2017 21 / 22

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SLIDE 24

Thanks

Meeran Zuberi (TIFR) Atmospheric Effects on GRAPES-3 July 13, 2017 22 / 22

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SLIDE 25

FFT Coefficient

C)

  • T (

10 − 8 − 6 − 4 − 2 − 2 4 6 8 10

I/I) % ∆ (

10 − 8 − 6 − 4 − 2 − 2 4 6 8 10

  • Det. 286

C

  • 0.005 % /

±

  • 1.254

Particle Density Vs Temperature

P (hPa) ∆

3 − 2 − 1 − 1 2 3

I/I) % ∆ (

2 − 1.5 − 1 − 0.5 − 0.5 1 1.5 2

  • Det. 286

0.005 % / hPa ±

  • 0.796

Particle Density Vs Pressure

Meeran Zuberi (TIFR) Atmospheric Effects on GRAPES-3 July 13, 2017 22 / 22

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SLIDE 26

Simulation

We have generated the 213 ( = 8192) sine wave hourly samples with 1 cycle / day periodicity. After performing FFT on the data a well spreaded power spectrum has been observed.

Time (Sec)

100 200 300 400 500 600 700

3

10 ×

Amplitude

2 − 1.5 − 1 − 0.5 − 0.5 1 1.5 2

Time Variation

Cycles/Day 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2

Amplitude

0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1

Power Spectrum

Meeran Zuberi (TIFR) Atmospheric Effects on GRAPES-3 July 13, 2017 22 / 22

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SLIDE 27

Temperature Vs Pressure

C

  • Temperature

5 10 15 20 25 Pressure (hPa) 774 776 778 780 782 784 786

Meeran Zuberi (TIFR) Atmospheric Effects on GRAPES-3 July 13, 2017 22 / 22

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SLIDE 28

Apart from pressure (2 cycle/day) & temperature (1 cycle/day) dominant cycles we can see other periodicity also in their power spectrums

Cycles/Day

1 2 3 4 5 6 7 8

Amplitude

0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2

Power Spectrum of Pressure

Cycles/Day

1 2 3 4 5 6 7 8

Amplitude

0.5 1 1.5 2 2.5 3 3.5 4

Power Spectrum of Temperature

Meeran Zuberi (TIFR) Atmospheric Effects on GRAPES-3 July 13, 2017 22 / 22

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SLIDE 29

Regression Method

The regression equation for two independent variable can be written as : Particle Density = a + b1 * Temperature + b2 * Pressure

Meeran Zuberi (TIFR) Atmospheric Effects on GRAPES-3 July 13, 2017 22 / 22

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SLIDE 30

Regression Method

6 months of air shower data (Jan to Jun, 2014) have been used for this study (same as FFT). Lag between particle density and temperature data has been calculated for all the detectors We have shifted the temperature data according to their lag for each detector.

Meeran Zuberi (TIFR) Atmospheric Effects on GRAPES-3 July 13, 2017 22 / 22

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SLIDE 31

Regression Method

Temperature Coefficient Distribution For All Detectors

Mean 0.8 − RMS 0.4778 Constant 6.15 ± 80.27 Mean 0.0225 ± 0.7308 − Sigma 0.0239 ± 0.3274

Temperature Coefficient

5 − 4 − 3 − 2 − 1 − 1 2 3 4 5

No of Detectors

10 20 30 40 50 60 70 80 Mean 0.8 − RMS 0.4778 Constant 6.15 ± 80.27 Mean 0.0225 ± 0.7308 − Sigma 0.0239 ± 0.3274

Mean = (-0.73 ± 0.02)%/◦C

Meeran Zuberi (TIFR) Atmospheric Effects on GRAPES-3 July 13, 2017 22 / 22

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SLIDE 32

Regression Method

Pressure Coefficient Distribution For All Detectors

Pressure Coefficient 2 − 1.5 − 1 − 0.5 − 0.5 1 1.5 2 No of Detectors 10 20 30 40 50 60

Pres_Coeff

Mean = (-0.54 ± 0.02)%/hPa

Meeran Zuberi (TIFR) Atmospheric Effects on GRAPES-3 July 13, 2017 22 / 22

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SLIDE 33

Regression Method

Temperature and Pressure Corrected Particle Density

Time (Sec)

100 200 300 400 500 600 700

3

10 ×

Particle Density

19000 20000 21000 22000 23000 24000 25000

Det#_2

Time variation

Cycles/Day 1 2 3 4 5 6 7 8 Amplitude 50 100 150 200 250 300 350 400 450 500

Det#_2

Power Spectrum

Meeran Zuberi (TIFR) Atmospheric Effects on GRAPES-3 July 13, 2017 22 / 22

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SLIDE 34

Coefficients Comparison

A close agreement has been found between the coefficient values from both the methods. % Pressure Coeff (/hPa) % Temperature Coeff(/◦C) FFT

  • 0.73 ± 0.01
  • 0.67 ± 0.02

Regression

  • 0.4 ± 0.02
  • 0.73 ± 0.02

Table : Coefficients comparison

Meeran Zuberi (TIFR) Atmospheric Effects on GRAPES-3 July 13, 2017 22 / 22