The versatile design is suitable for various applications, including MOKE (Magneto-Optic Kerr Effect) materials analysis, variable temperature optical cryostats, Hall probe calibration and vibrating sample magnetometer (VSM) systems.
HTS-110’s dipoles are extensively utilised in the commercial development of hard-drive components, with the high magnetic field and fast ramp rates which facilitates high throughput of next generation materials.
Model |
Peak field (T) |
Pole gap (mm) |
Sample access slot (mm) |
Mass (kg) |
Ramp time 4-quadrant (s) |
XT (standard) |
|
|
|
|
|
5XT |
5 |
26-34 |
26 x 80, Φ30 |
|
~900 |
8XT |
8 |
26-34 |
26 x 80, Φ30 |
670 |
~1200 |
|
|
|
|
|
|
XR “rapid” (fast-ramping) |
|
|
|
|
|
7XR05 |
7 |
5 |
18 x 130 |
520 |
305 |
|
|
|
|
|
|
XE “express” (faster ramping) |
|
|
|
|
|
5XE10 |
5 |
10 |
14 x 120 |
250 |
80 |
6XE03 |
6 |
3 |
14 x 120 |
250 |
80 |
|
|
|
|
|
|
XU “ultrafast” (fastest ramping) |
|
|
|
||
7-8XU03 |
7/ 8 |
3 |
8 x 110 |
375 |
62 (7 T) / 200 (8 T) |
* Note: XR, XE and XU magnets have optional optical access along the pole axis.