HAT-P-13b is a Jupiter-mass transiting exoplanet that has settled onto a stable, short-period, and mildly eccentric orbit as a consequence of the action of tidal dissipation and perturbations from a second, highly eccentric, outer companion. Owingto the special orbital configuration of the HAT-P-13 system, the magnitude of HAT-P-13bʼs eccentricity (e b ) is in part dictated by its Love number (k 2 b ), which is in turn a proxy for the degree of central mass concentration in its interior. Thus, the measurement of e b constrains k 2 b and allows us to place otherwise elusive constraints on the mass of HAT-P-13bʼs core (M core,b ). In this study we derive new constraints on the value of e b by observing two secondary eclipses of HAT-P-13b with the Infrared Array Camera on board the Spitzer Space Telescope. We fit the measured secondary eclipse times simultaneously with radial velocity measurements and find that e b =0.00700±0.00100. We then use octupole-order secular perturbation theory to find the corresponding = Applying structural evolution models, we then find, with 68% confidence, that M core,b is less than 25 Earth masses (M ⊕ ). The most likely value isM core,b =11 M ⊕ , which is similar to the core mass theoretically required for runaway gas accretion. This is the tightest constraint to date on the core mass of a hot Jupiter. Additionally, we find that the measured secondary eclipse depths, which are in the 3.6 and 4.5 μm bands, best match atmospheric model predictions with a dayside temperature inversion and relatively efficient day-night circulation.