Title: B V Sreekantan
 1B V Sreekantan
Front Ranking Cosmic Ray Experiments carried out 
in the late 40s and 50s at TIFR with Home-Made 
Detectors and Electronics
Panel Discussion, TIFR, Mumbai 15 January 2010 
 2Mu-meson Life Time and decay spectrum (1948-51)  BVS Harold Tycho working under Prof. Rossi  publishes his results in Phys. Rev. Microsecond Electronics Triggered Oscilloscope Pulsed Circuits Iron Magnet All with military disposal valves brought from Chor Bazar GM counters with double-distilled alcohol as quenchers. (Nucleonic Elmore and Sands) 
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 5Experimental arrangement II Positive mesons 
focussed into the paraffin absorber in which they 
decay, by the magnetic lens M. 
 6Typical oscilloscopic records of the ?-meson 
decay events registered. 
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 8KGF Experiments 1st phase 1951 onwards. First Elementary Particle Conference in Bombay, Dec. 1950 KGF 2nd phase Ratio of ks to Pis (1951-53) 1954  Khandala Cloud Chamber in Railway Tunnel (200 ft) 18 cloud chamber built in TIFR workshop Intensity-Depth upto 1000 ft with Hodoscoped Telescope (BVS  SN) Bhabha suggets to verify whether all underground particles are muons Angular Distribution of muons at various Depths. Cloud Chamber at depth of 100 ft in search of APPs (BVSSNPVR) ABSBVSSNPVR Search of APPs continued. 
 91954-55 MIT  Echo Lake Cambridge (Mass.) HP 327 Oscilloscope Nanosecond timing made possible. Bhabha orders even before my return. Book Millimicrosecond Pulse Techniques S-particles (k?2 , k?3) 
 10- Development of Chronotron  Measurement of 
 Nanosecond Timing for Air Shower Experiments
- Scintillation Counter for EAS  Bombay TIFR 3rd 
 Floor
-  Ooty Raj Bhavan 
- Rani and Maharani Cloud Chambers at Ooty- 
 S-particle Searches
- Development of Spark Counters 
-  Cores of Extensive Air Showers 
- Development of Total Absorption Spectrometer 
 (TASS)
- Triple setup Cloud Chamber  Air Cerenkov 
 Counter  TASS
- Large Cloud Chamber  Largest in the World 
 (Miyake)
11Photograph of a completely assembled spark 
counter (a) aluminium angles to keep the plastic 
frame straight (b) plastic frame 60 cm x 30 cm 
(c) stainless steel plate 50 cm x 30 cm x 3 mm 
(d) brass welding rods 58 cm long, 3 mm diameter. 
 12Experimental arrangement to test the feasibility 
of employing nuclear emulsions in conjunction 
with double spark counter array for the study of 
high energy jets. The coincidence G1SG2 selects 
nuclear interactions produced mostly in the water 
tank. The lead plates above the spark counter are 
meant for the rapid development of the cascades. 
The direction and co-ordinates of the jets are 
given by the position of the sparks in the two 
spark counters. 
 13Photograph of a typical double spark event. The 
sparks have occurred (shown AA) in the right 
extreme compartment in both the counters. The 
bright strips seen in the photograph correspond 
to the portions of brass rods below the ribs of 
the plastic frame illuminated for a short time, 
immetiately after photographing the sparks but 
before advancing the film. This serves as a 
convenient reference frame for locating sparks.  
 14Cloud chamber photograph of a high energy 
penetrating shower proceed in the lead block 
above the chamber and developing further in the 
lead plates side. A spark was seen in the spark 
counter in the region through which the axis of 
the shower passed the spark counter. 
 15An enlarged view of the section of two adjacent 
layers of the spectrometer showing the details of 
design of the liquid scintillation tank. 
 16A cross sectional view of the total absorption 
scintillation spectrometer (TASS) and the shower 
detector. 
 17Schematic diagram of the chronotron system for 
measurement of arrival time of the hadrons signal 
from TASS relative to the signal from the shower 
detector CHO. 
 18A block diagram of the circuitry associated with 
the spectrometer. 
 19Comparison of the observed time spectra for 
hadrons of (10 ? 20 GeV energy with spectra 
calculated using different models of high-energy 
hadron collisions. The statistical errors as well 
as the errors in the measured arrival time are 
shown on each experimental point except the 
aero-time point which is free of timing errors. 
 Is the average shower size and R is the 
distance of the hadron from shower axis,  
102, R ? 20 m. ? experimental data --------- 
calculations. 
 20Triple arrangement of Air Cerenkov Counter, 
Multiplate Cloud Chamber and Total Absorption 
Spectrometer at Ooty, for the study of 
interactions of pions and protons in 10-100 GeV 
range. 
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 22Core Regions of Extensive Air Showers
A cascade which develops from the first plate of 
the chamber and shows a rapid absorption after 
the maximum. The method of cascade widths has 
been used for energy estimation which is 750 GeV.
Several cascades having elongated tube-like 
structures not completely absorbed even after 20 
radiation lengths. The estimated energy of the 
largest cascade is 2.4 TeV. 
 23- Ooty Team 
- BVS  SN  AS  PVR  SL  SDV  TNR  GTM  BKC 
 MVS  RR  RHV  SCT
-   (Miyake) 
- Dinshaw  Apte  Khairatkar  Kalagaonkar  
 Gonsalves  Manchanda  Gopal
- KGF Team 
-  BVSSN MVS  PRV  KS  VSN  MGK  KA  
 British  Japanese
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