Kondo physics in doped monolayer graphene is predicted to exhibit unusual
features due to the linear vanishing of the pristine material's density of
states at the Dirac point. Despite several attempts, conclusive experimental
observation of the phenomenon remains elusive. One likely obstacle to
identification is a very small Kondo temperature scale TKβ in situations
where the chemical potential lies near the Dirac point. We propose tailored
mechanical deformations of monolayer graphene as a means of revealing unique
fingerprints of the Kondo effect. Inhomogeneous strains are known to produce
specific alternating changes in the local density of states (LDOS) away from
the Dirac point that signal sublattice symmetry breaking effects. Small LDOS
changes can be amplified in an exponential increase or decrease of TKβ for
magnetic impurities attached at different locations. We illustrate this
behavior in two deformation geometries: a circular 'bubble' and a long fold,
both described by Gaussian displacement profiles. We calculate the LDOS changes
for modest strains and analyze the relevant Anderson impurity model describing
a magnetic atom adsorbed in either a 'top-site' or a 'hollow-site'
configuration. Numerical renormalization-group solutions of the impurity model
suggest that higher expected TKβ values, combined with distinctive spatial
patterns under variation of the point of graphene attachment, make the top-site
configuration the more promising for experimental observation of signatures of
the Kondo effect. The strong strain sensitivity of TKβ may lift top-site
Kondo physics into the range experimentally accessible using local probes such
as scanning tunneling microscopy.Comment: 19 pages, 7 figures (added Figs. 6 and 7 to version 1