By using intense laser irradiating a micro plane target obliquely, an enhanced γ-ray source is generated. Due to the superposition of the incident and the reflected laser pulses, electron bunches with density of ∼300nc are extracted and accelerated. When these electron bunches separate from the edge of the target that the laser is leaving, they co-propagate with the laser field and emit dense γ-rays simultaneously. Simulation results show that the emitted γ photons are 253nc dense with an averaged energy of ∼12 MeV. The yield of γ photons is ∼7 × 1012, achieving a high brightness of ∼4 × 1023. Influences of the laser intensity and the incident angle on the γ-rays emission are discussed. The γ-ray yield, the conversion efficiency from the laser to the γ-rays and the averaged γ-ray energy are increasing when irradiating a higher intensity laser. With the increasing of the incident angle, the peak photon density increases when the angle is smaller than 20° and then drops to a stable value, while the divergence decreases when the incident angle is smaller than ∼16° and then increases.