|Magnet Type:||2 x Helmholtz, 1 x Saddle|
|Field Strength/Orientation:||0.3 T / z, 20 mT / x, 20 mT / y|
|Field Calibration:||0.000425 T/A (4.25 G/A) z|
0.0000341 T/A (0.341 G/A) x
0.000119 T/A (1.19 G/A) y
|Counter acceptance:||4 π|
|Experiment types:||LF, TF, LTF, ZF, RF-microwave|
Omni was so successful that there was demand for a copy of it, and less demand for an existing spectrometer named Eagle. Eagle was stripped of its main coils which were used to build another Omni apparatus, Omni', which was later rebuilt to its current configuration.
The main coils are spaced a generous 13.3 cm apart, providing 3.2 kG (0.32 T) axially with 750 A (4.25 G/A). There is a pair of Helmholtz coils for 150 G vertical field and saddle coils within the main magnet bore providing up to 200 G horizontal transverse field. Furthermore, there are axial shim coils for active feedback field control, as well as three-axis square coils for zeroing the field.
Several counter and sample-holder arrangements are possible using three side-tables and top platform. (The latter has easy access via a staircase.)
Omni' is used exclusively for higher energy backward muons (on M9B). To this end it has a lead collimator wall, 3 inches thick, upstream of the coils, and two 1-inch copper collimator walls sliding on a track within the coils. This arrangement may need some explanation. For backward muons, it is desirable to use two muon counters, in coincidence, to avoid counting x-rays and positrons, and there should be collimation between the two counters so that they do not count decay positrons as beam muons. In the case of Omni', the first counter, M0, is inserted between the lead and copper walls while the second goes after all collimation, just before the sample. Note that all collimators take tungsten inserts to select the size of hole, though the holes in the upstream collimators should be larger.