Cosmic Ray Observatory Project Fr Michael LieblAGU Conference Mount Michael Benedictine High SchoolDecember 6, 2005 Elkhorn Ne 68022

ca Austrian physicist Victor Hess of the Vienna University discovered ionizing radiation in a series of hydrogen balloon flights.

ca Robert Millikan of Caltech in collaboration with Ira Bowen made high-altitude measurements which confirmed the existence of what Millikan coined “cosmic rays.”

A eV cosmic ray air shower can yield 100 billion particles at sea level, most of which are muons, photons and electrons

Dr. Greg Snow Dr. Dan Claes P [78 of 84]

Illustration courtesy Lincoln Journal Star

PROJECT GOALS Educational: Train teams of high school teachers and students to study cosmic rays Scientific: Build a statewide network of cosmic ray detectors Search for the sources of ultra-high energy cosmic rays

The Cosmic Ray Spectrum

Chicago Air Shower Array (CASA)

Photo courtesy U. S. Army

Charged particle passing through scintillator panel produces light which is detected by photomultiplier tube (PMT) Photomultiplier tube Scintillator panel

Oscilloscope trace of signal from photomultiplier tube

2000: Lincoln Zoo School, Lincoln Northeast, Mount Michael, Marian, Norfolk 2002: Fairbury, Wayne, Roncalli Catholic, Bancroft-Rosalie, Waterloo 2001: Lincoln Lutheran, Lincoln High, Westside, Anselmo-Merna, Osceola, Wayne State College 2003: Coleridge, Loup, McPherson, Mullen, Spalding

2004: Lincoln Pius X, Scottsbluff, Keya Paha, Madison, Westside II 2004: Lincoln Southwest

Disassembly of scintillator panel from CASA experiment

Cleaning and polishing scintillator panels

Gluing photomultiplier tubes onto scintillator panels

Wrapping scintillator panels with aluminum foil

Re-taping black cover over refurbished scintillator

Testing scintillator panels and photomultiplier tubes

Learning to use an oscilloscope for the study of cosmic rays

Scintillator panel and photomultiplier tube in weatherproof box ready to be placed on roof of school

Barometric Pressure (mmHg) Fold Coincidences / 2 hours Study by Marian High School of Count Rate versus Barometric Pressure

The Science Teacher November 2001 Vol. 68 No. 8

5 Volt DC power PC serial port Four analog PMT inputs Discriminator threshold adjust GPS receiver input Programmable logic device Time-to-digital converters Developed by Univ. Nebraska, Fermilab (Quarknet), Univ. Washington CROP Data Acquisition Electronics Card (DAQ) Event counter 43 MHz (24nsec) clock interpolates between 1 pps GPS ticks for trigger time TDC’s give relative times of 4 inputs with 75 picosecond resolution

Labview Software for PC control of DAQ card

Summer 2005 Workshop Bring participating schools to Lincoln campus Refresh skills on use of equipment Replace damaged or non-functioning equipment Proof of principle experiment

Summer 2005 Workshop

Challenges Distances between schools are large Replacement or repair of equipment Rural schools sometimes have no physics teacher Rural schools may have physics teachers teaching out of discipline Replacing trained students Support of local school administration Maintaining enthusiasm over prolonged time span

A Threshold Scan Rather than focusing on a single fit to the entire range of data, recognize that two different physics processes are at play. Both generate counts, but with rates that drop off differently with increasing threshold. (Both drop ~exponentially, which is why we resort to the logarithmic plot). At LOW THRESHOLD we expect to be dominated by noise, which plummets rapidly with threshold. Its exponential drop should ideally look like a straight line on a logarithmic plot. At HIGH THRESHOLD the background noise should be pretty much eliminated, and any additional increase in threshold will actually start cutting into the real signal. Real signals are, on average, hardier, so the drop is less severe. This defines two regions with relatively flat (linear) response. Because of the statistical fluctuates common in random events like noise or cosmic ray counts, how straight the lines are may depend on how long you ran at each data point (at least minutes should be OK). Of course the two regions overlap, so there's a middle region that curves. But we can focus on the first few points at each extreme to determine our linear fits, as I have done (by eye) above. We use the intersection of the two lines to select the threshold (which looks to be about 65 mV in the example above to me). It's a nice to try and confirm your selection by eye. Recall you can set trigger threshold on the oscilloscope. A very low threshold will have the oscilloscope almost continuously triggering, revealing a band of noise (see above). Moving the threshold just far enough to kill the noise and give only the flickering images of healthy signals can give you an approximate idea of where the threshold should be set. See if you can confirm this sort of behavior for the setting your scans suggest you use. Recall the DAQ card has a built-in x2 amplifier, so uses thresholds twice the size of the ones you'll need for the oscilloscope trigger (i.e., a threshold of 65mV from the DAQ card scan corresponds to a 32mV trigger threshold on the oscilloscope). Sample of Web Based Help Page

FUTURE Duplicate 2005 workshop experiment with detectors on school rooftops Begin integration of results from dispersed detectors Bring more schools on line Secure additional funding for the future of CROP Coordinate activities with other high school cosmic ray projects CROP Website