Abstract. Interstellar medium clouds in the W28 region are emitting gamma-rays and it is likely that the W28 supernova remnant is responsible, making W28 a prime candidate for the study of cosmic-ray acceleration and diffusion. Understanding the influence of both supernova remnant shocks and cosmic rays on local molecular clouds can help to identify multi-wavelength signatures of probable cosmic-ray sources. To this goal, transitions of OH, SiO, NH 3 , HCO + and CS have complemented CO in allowing a characterisation of the chemically rich environment surrounding W28. This remnant has been an ideal test-bed for techniques that will complement arcminute-scale studies of cosmic-ray source candidates with future GeV-PeV gamma-ray observations.
The W28 RegionW28 is an old-age (>10 4 years, see [1,2,3]) supernova remnant (SNR), which exhibits non-thermal synchrotron emission seen in 90 cm radio continuum in Figure 1. The W28 SNR has been implicated as a cosmic ray (CR) accelerator due to a correspondence between TeV gamma-ray emission and molecular gas at a distance of 1.2-3.3 kpc [4,5,6,7]. This correspondence is true of both HESS J1801−233 -a TeV gamma-ray source immediately adjacent/overlapping the SNR, and HESS J1800−240 -a multi-component TeV gamma-ray source spatially separated by 0.25-0.75• in the plane of the sky. Such gamma-ray-gas overlap points to gamma-ray emission via the decay of neutral pions created by CR interactions with gas. It follows that the W28 SNR is a likely cosmic-ray accelerator [8,9,5]. Some uncertainty exists in the 3D geometry of the cloud complex surrounding W28 and the energy-dependent diffusion speed of CRs throughout that region. But, successive multi-wavelength campaigns have reinforced evidence for a SNR-cloud interaction and supported a hadronic scenario for gamma-ray emission.
The Shocked Molecular Cloud towards HESS J1801−233As illustrated in Figure 2, CO-traced molecular gas [10,11,5] between kinematic velocities 0 and 20 kms −1 corresponds to the TeV gamma-ray emission of HESS J1801−233. A component of shock-heated molecular gas is seen in H 2 [12,13] and high-J CO transitions [10] along the radio-continuum-traced W28 shock, while 1720 MHz OH masers (indicated in Figure 2) are also encompassed within this velocity-range [14,15]. 1720 MHz OH maser lines are commonly associated with the wake of old ( 10 4 yr) supernova remnant shocks (e.g.[15]), and modelling suggests that very specific collisional conditions are required for their generation [16,17,18]. C-type shocks (∼25 kms −1 ) moving through dense (∼10 4 -10 5 cm −3 ), warm (50-125 K) molecular gas can sustain OH maser emission provided that a source of H 2 O-dissociation is present to maintain a large OH column density (∼10 16 cm −2 ), possibly a weak UV flux emitted by H 2 that has been indirectly excited by CRs and/or X-ray photons [19].