TIEN-SHAN FUTURE PRESENT PASTS

Similar documents
Primary cosmic ray mass composition above 1 PeV as measured by the PRISMA-YBJ array

Primary CR Energy Spectrum and Mass Composition by the Data of Tunka-133 Array. by the Tunka-133 Collaboration

John Ellison University of California, Riverside. Quarknet 2008 at UCR

Ashot Chilingarian Artem Alikhanyan National Laboratory (Yerevan Physics Institute)

Vasily Prosin (Skobeltsyn Institute of Nuclear Physics MSU, MOSCOW) From TAIGA Collaboration

The Physics of Cosmic Rays

TeV energy physics at LHC and in cosmic rays

Publications of Francesco Arneodo: journal articles

Very High Energy Gamma Ray Astronomy and Cosmic Ray Physics with ARGO-YBJ

LATTES Large Array Telescope to Tracking Energetic Sources

Timing calibration of the LHAASO-KM2A electromagnetic particle detectors

Cosmic Rays in the earth s atmosphere. Ilya Usoskin Sodankylä Geophysical Observatory ReSoLVE Center of Excellence, University of Oulu, Finland

The KASCADE-Grande Experiment

Detectors for astroparticle physics

Neutron flux measurement using fast-neutron activation of 12 B and 12 N isotopes in hydrocarbonate scintillators

A SEARCH FOR ASTROPHYSICAL POINT SOURCES OF 100 TEV GAMMA RAYS BY THE UMC COLLABORATION

Observation of UHECRs in horizontal flux

Mass Composition Study at the Pierre Auger Observatory

Neutron Induced Nuclear Counter Effect in Hamamatsu Silicon APDs and PIN Diodes

Status KASCADE-Grande. April 2007 Aspen workshop on cosmic ray physics Andreas Haungs 1

Study of Performance Improvement for Air Shower Array with Surface Water Cherenkov Detectors

Neutrino Astronomy. Ph 135 Scott Wilbur

Neutrino induced muons

High-energy neutrino detection with the ANTARES underwater erenkov telescope. Manuela Vecchi Supervisor: Prof. Antonio Capone

Numerical study of the electron lateral distribution in atmospheric showers of high energy cosmic rays

Cherenkov Detector. Cosmic Rays Cherenkov Detector. Lodovico Lappetito. CherenkovDetector_ENG - 28/04/2016 Pag. 1

Experimental Particle Physics

Cosmic Rays: A Way to Introduce Modern Physics Concepts. Steve Schnetzer

Experimental Particle Physics

Study of Charm Production in Forward Cone at Energy E Lab 75 TeV with two-storey XREC Exposed at Mountain Altitudes

Air Shower Measurements from PeV to EeV

Calorimetry in particle physics experiments

STUDY OF EXTENSIVE AIR SHOWERS IN THE EARTH S ATMOSPHERE

The Multiple Muon Charge Ratio in MINOS Far Detector

PoS(ICRC2015)424. YAC sensitivity for measuring the light-component spectrum of primary cosmic rays at the knee energies

Neutrinos with a cosmic ray detector. Cosmic rays with a neutrino detector

7 th International Workshop on New Worlds in Astroparticle Physics São Tomé, September 2009 THE AMIGA PROJECT

arxiv:physics.ins-det/

Detecting High Energy Cosmic Rays with LOFAR

9/27 JUNE 2003 SUMMER STAGE PARTICLES REVELATION THROUGH CERENKOV AND SCINTILLATION COUNTER AND THE CEBAF EXPERIMENT

Radiation (Particle) Detection and Measurement

Thin Calorimetry for Cosmic-Ray Studies Outside the Earth s Atmosphere. 1 Introduction

Windows on the Cosmos

Cosmic ray studies at the Yakutsk EAS array: energy spectrum and mass composition

PARTICLES REVELATION THROUGH SCINTILLATION COUNTER

The early days of ground-based gamma-ray astronomy in France. Gerard Fontaine - Hillas symposium Heidelberg December

Extensive Air Showers and Particle Physics Todor Stanev Bartol Research Institute Dept Physics and Astronomy University of Delaware

IceCube. francis halzen. why would you want to build a a kilometer scale neutrino detector? IceCube: a cubic kilometer detector

The TAIGA experiment - a hybrid detector for very high energy gamma-ray astronomy and cosmic ray physics in the Tunka valley

High energy neutrino astronomy with the ANTARES Cherenkov telescope

Interaction of particles in matter

GAMMA-RAY ASTRONOMY: IMAGING ATMOSPHERIC CHERENKOV TECHNIQUE FABIO ZANDANEL - SESIONES CCD

Particle Physics Beyond Laboratory Energies

Beam diagnostics: Alignment of the beam to prevent for activation. Accelerator physics: using these sensitive particle detectors.

Recent Results from the KASCADE-Grande Data Analysis

Cosmic Rays. Discovered in 1912 by Viktor Hess using electroscopes to measure ionization at altitudes via balloon

Calibration of large water-cherenkov Detector at the Sierra Negra site of LAGO

AugerPrime. Primary cosmic ray identification for the next 10 years. Radomír Šmída.

Some Thoughts on Laboratory Astrophysics for UHE Cosmic Rays. Pierre Sokolsky University of Utah SABRE Workshop SLAC, March, 2006

The JUNO veto detector system. Haoqi Lu Institute of High Energy physics (On Behalf of the JUNO Collaboration) TIPP2017, May22-26,Beijing

ATLAS Hadronic Calorimeters 101

Parameters Sensitive to the Mass Composition of Cosmic Rays and Their Application at the Pierre Auger Observatory

Experimental studies of East-West effect of the charge ratio of atmospheric muons with energies relevant to the atmospheric neutrino anomaly

SUPPLEMENTARY INFORMATION

Review of Particle Properties: ( ). See the review section on Cosmic Rays under Astrophysics and Cosmology.

SiPM & Plastic Scintillator

Cosmic Rays II. CR observation Air and space based experiments Underground. experiments. experiments. Ground based. Astroparticle Course 1

Verification of the CORSIKA code in the TeV energy

Experimental Particle Physics

Cosmic ray indirect detection. Valerio Vagelli I.N.F.N. Perugia, Università degli Studi di Perugia Corso di Fisica dei Raggi Cosmici A.A.

Cosmic Rays - in Poland

Cosmic Rays and the need for heavy payloads

American Institute of Physics 207

From the Knee to the toes: The challenge of cosmic-ray composition

Chapter 6.2: space based cosmic ray experiments. A. Zech, Instrumentation in High Energy Astrophysics

TAIGA-HiSCORE results from the first two operation seasons

Educational cosmic ray experiments with Geiger counters

A Multimessenger Neutrino Point Source Search with IceCube

High Energy Neutrino Astronomy

Optic Detectors Calibration for Measuring Ultra-High Energy Extensive Air Showers Cherenkov Radiation by 532 nm Laser

The Pierre Auger Observatory and ultra-high energy neutrinos: upper limits to the diffuse and point source fluxes

TGE terminated by lightning at the maximum of the flux; red disturbances of electrostatic field; blue distance to lightning (~2 km); green small

Indirect Dark Matter Detection

On the possibility to forecast severe radiation storms by data from surface and space-born facilities

Complex set of cosmic rays monitoring

The LHAASO-KM2A detector array and physical expectations. Reporter:Sha Wu Mentor: Huihai He and Songzhan Chen

OVERVIEW OF THE RESULTS

X- & γ-ray Instrumentation

PoS(ICRC2017)462. Cherenkov differential detector at the Yakutsk extensive air shower array

Applied Nuclear Physics (Fall 2006) Lecture 21 (11/29/06) Detection of Nuclear Radiation: Pulse Height Spectra

Exploring the Lifetime Frontier and Cosmic Ray Physics

The Cosmic Ray Mass Composition in the Energy Range ev measured with the Tunka Array: Results and Perspectives

1. Introduction on Astroparticle Physics Research options

IceCube: Dawn of Multi-Messenger Astronomy

Temperature Dependence Calibration and Correction of the DAMPE BGO Electromagnetic Calorimeter

Limits on Antiprotons in Space from the Shadowing of Cosmic Rays by the Moon

Gamma-Ray Astronomy with a Wide Field of View detector operated at Extreme Altitude in the Southern Hemisphere.

Dark Matter Particle Explorer: The First Chinese Cosmic Ray and Hard γ-ray Detector in Space

Search for EeV Protons of Galactic Origin

Measuring the neutrino mass hierarchy with atmospheric neutrinos in IceCube(-Gen2)

Transcription:

TIEN-SHAN PASTS PRESENT FUTURE

TIEN SHAN MOUNTAIN STATION OF P.N. LEBEDEV INSTITUTE DISPOSES AT THE DISTANCE OF 46 KM FROM THE BIG ALMA-ATA ATA CITY AT 3340 m ABOVE SEA LEVEL

THE BIG ALMA-ATA LAKE AND THE ROAD TO THE STATION

TIEN-SHAN: PAST

The first complex array at Tien-Shan (1965-1970) 1, 4 - Geiger counters 2 - Li H target 3 - Cloud chamber in magnet field 5 - Ionization calorimeter THE MAIN RESULT: FINDING OF DISSIMETRICAL SHOWERS AT ENERGIES 60-1000 GeV

PRESIDENT OF SOVJET ACADEMY OF SCIENCIES M.V.KELDYSH ACQUAINTS WITH THE CLOUD CHAMBER ARRAY (1966)

COMPLEX ARRAY FOR EAS STUDY (1966-1982) 1982) 180 м 38 м 73 м -Calorimeter 36 m 2 - µ-array

HADRON ARRAY (1985-19 1991) - Cherenkov Detectors - Scintillator detectord - Geiger counters A - X-ray emulsion chamber and ionization bursts array µ Muon array - Detector of Cherenkov pulse shape

COSMIC RAYS ENERGY SPECTRUM INVESTIGATION

10 5 10 4 10 3 10 2 10 1 NUMBER OF EVENTS

THE BIG IONIZATION CALORIMETER

TSIC had an area of 36 m 2 and consisted of 15 (finally - 19) rows of copper ionization chambers of sizes 5,5 24 300 cm 3. Each row contained 48 ionization chambers. The total thickness of lead absorber (including the thickness of chamber walls and steel carcass recalculated to lead) was equal to 850 g/cm2 (1000 g/cm 2 finally). Each chamber had its own ADC with a dynamical range 2.10 4. The signal measuring accuracy was better than 10% over the total range. The signal from a chamber was memorized in the diode-capacitor cells whereupon the series of growing pulses was fed to all ADС inputs. Each next pulse in the series was 10% greater than previous one. The first pulse with an amplitude being 10% greater than that of memorized one passed through the diode-capacitor cell and its number n was fixed. All ADC s were calibrated in such a way after each trigger pulse. The calorimeter operation control has included the daily statisti-cal analysis of each channel: its amplitude spectrum was compared with a spectrum derived by averaging over all the chambers of the given specific row.

DISTRIBUTION OF ELASTICITY COEFFICIENT AT E=2 TeV RESTORED WITH THE USAGE OF INVERSE PROBLEM (1975) Experiment MQ 1 U p,n dn/du p,n 0,1 0,0 0,2 0,4 0,6 0,8 1,0 U p,n

THE LONG FLYING COMPONENT

1100 1000 900 800 700 λ (E), g/cm 2

EVENTS WERE SEPARATED ACCORDING TO THE SIGN OF b c VALUE NGTH L(E), g/cm 2 2000 1500 calc [ b c b c <

EVENTS WITH b c >0 WERE COMPARED WITH M-C CALCULATIONS IN ASSUMPTION OF 100% Λ c + D IN THE FIRST INTERACTION NGTH L(E), g/cm 2 4000 3000 Monte-C Experim

AVERAGED CASCADES IN THE CALORIMETER NORMALIZED TO EAS SIZE JUMP LIKE DECREASE AT PRIMARY ENERGY ABOVE 10 16 ev < I(x,N e ) / N e > 10

ENERGY OF GAMMA FAMILIES NORMALIZED TO PRIMARY ENERGY JUMP LIKE DECREASE AT ENERGY ABOVE 10 16 ev 0.01 E γ / E 0, per family 0.005

CHERENKOV ARRAY CHERENKOV LIGHT FLUX IS THE MOST ADEQUATE MEASURE OF SHOWER ENERGY

CHERENKOV DETECTORS

EAS SIZE NORMALIZED TO SHOWER ENERGY JUMP LIKE DECREASE AT ENERGY ABOVE 10 16 ev 4x10-5 3x10-5 N e / E 0 2x10-5

MUON NUMBER NORMALIZED TO PRIMARY ENERGY JUMP LIKE INCREASE AT ENERGY 10 16 ev 3.0x10-12 N µ / E 0 2.5x10-12 2.0x10-12

TIEN-SHAN PRESENT

TODAY TRIGGERING SYSTEMS

INVESTIGATION OF NEUTRONS IN EAS

TIME DELAY OF NEUTRONS AFTER EAS FRONT AT DIFFERENT NEUTRON MULTIPLICITY background µs

DISTRIBUTIONS OF NEUTRONS RECIPROCAL DELAY TIME AT DIFFERENT NEUTRON MULTIPLICITY µs -1

SPECTRA OF NEUTRON MULTIPLICITY AT DIFFERENT DEPTH OF OBSERVATION EVIDENCE OF UNSTABLE COMPONENT

In EAS with energy 10 15 ev delaying penetrating particles with time delay 60ns relative to shower front was found in the underground scintillator array (MUON-T).

IONIZATION-NEUTRON CALORIMETER WITH TWO-STORIED X-RAY FILM EMULSION CHAMBER WITH AIR GAP

EXPERIMENTUM CRUCIS TIEN-SHAN 2005 Expected PAMIRS 1987 casc.units

THE FIRST GAMMA TELESCOPE

THE SECOND GAMMA TELESCOPE

INVESTIGATION OF NEUTRINO OSCILLATIONS WITH USAGE OF EAS PRODUCED IN MOUNTAIN INVESTIGATION OF LOCAL GAMMA RAY SOURCES

INVESTIGATION OF THUNDESTORMS AND THEIR CORRELATIONS WITH EAS

EXAMPLE OF CHARGED CLOUD PASSAGE ABOVE THE NOTCH

TIEN-SHAN FUTURE

COMPLEX ARRAY ATHLET (ALMATY THREE LEVEL EXPERIMENTAL TECHNICS)

Second center with INCA

SHOWER ARRAY ALLOCATED AT 30 DEGREES TO ZENITH WILL DETECT IN EQUAL CONDITIONS VERTICAL EAS, SO AS SHOWERS INCLINED TO 60 0 AND RESOLVE THE OLD PUZZLE ON ALTITUDE DEPENDENCE OF KNEE POSITION. ALTITUDE DEPENDENCE OF KNEE POSITION

SCHEMATIC DROWING OF THE SECOND CENTER WITH INCA ARRAY

THE MAIN GOALS OF THE EXPERIMENT 1. Searching of the correlations between different anomalous phenomena in EAS. 2. Eduction of the role of anomalous phenomena in the energetics of nuclearcascade process and redistribution of primary particle energy between different EAS components. 3. Investigation of the reliability of modern QGS (and other) models for recalculations from measured values of EAS parameters N e and N µ to the primary energy Е 0. 4. Investigation of the influence of anomalous phenomena on the restitution of primary cosmic rays energy spectrum and mass composition. 5. Do unusual particles (like strangelets, WIMP, etc) exist in the primary cosmic rays and can they be the reason of anomalous phenomena in EAS cores?

COME TO ALMA-ATA ATA CITY ON AUGUST 25-27 27 2006 TO ATTEND INTERNATIONAL WORKSHOP TIEN-SHAN 2006 Contact: yakovlev@sci.lebedev.ru