Cerenkov technology is often the optimal choice for particle identification
in high energy particle collision applications. Typically, the most challenging
regime is at high pseudorapidity (forward) where particle identification must
perform well at high high laboratory momenta. For the upcoming Electron Ion
Collider (EIC), the physics goals require hadron ($\pi$, K, p) identification
up to $\sim$~50 GeV/c. In this region Cerenkov Ring-Imaging is the most viable
solution.\newline The speed of light in a radiator medium is inversely
proportional to the refractive index. Hence, for PID reaching out to high
momenta a small index of refraction is required. Unfortunately, the lowest
indices of refraction also result in the lowest light yield
($\frac{dN_\gamma}{dx} \propto \sin^2{\left(\theta_C \right)}$) driving up the
radiator length and thereby the overall detector cost. In this paper we report
on a successful test of a compact RICH detector (1 meter radiator) capable of
delivering in excess of 10 photoelectrons per ring with a low index radiator
gas ($CF_4$). The detector concept is a natural extension of the PHENIX HBD
detector achieved by adding focusing capability at low wavelength and adequate
gain for high efficiency detection of single-electron induced avalanches. Our
results indicate that this technology is indeed a viable choice in the forward
direction of the EIC. The setup and results are described within.Comment: 10 pages, 15 figure