For an aperture with transverse size D, Fraunhofer region is named when the distance between the aperture and the detector is larger than D 2 / , where is the wavelength of the illuminating light. For a lensless system, when both reference detector and the object are located in Fraunhofer region relative to the thermal source, we demonstrate that a ghost "pinhole" camera with magnification M = z / z 1 can be obtained by the second-order correlation of two light fields even if the test detector is a single pointlike detector. Effects determining the quality of ghost pinhole imaging and its potential applications are also discussed. © 2009 American Institute of Physics. ͓DOI: 10.1063/1.3207832͔For conventional lensless optical system, as shown in Fig. 1, when the thermal light from an object goes through a pinhole, a true image with the magnification M = z 0 / z 1 can be obtained if a charge-coupled device ͑CCD͒ camera is positioned in the Near-contact region. This imaging process is called pinhole imaging, which is widely used in x-ray and neutron imaging. Projection imaging system without limit to the depth of light field, such as pinhole imaging, is very useful in many applications, for example, security inspection. Based on the first-order correlation of light field and the light propagating as a straight line in Near-contact region, pinhole imaging is the only lensless projection imaging scheme realizing a true image with magnification M Ͼ 1. When the CCD camera is positioned in Fraunhofer region ͑R Ͼ D 2 / , see Fig. 1͒ because of diffraction effect of the pinhole, it is impossible to achieve true image of the object by lensless pinhole imaging system. Different from conventional pinhole imaging method, ghost imaging, based on the second-order correlation of light fields, can nonlocally image an object by two-photon interference involving a joint detection of two photons at distant space-time points with both entangled source and thermal light. [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15] In this letter, a lensless ghost pinhole camera is investigated when both the object and the reference detector, relative to the thermal source, are located in Fraunhofer region.In previous lensless ghost imaging systems, the object is adjacent to the test detector, so the test detector should be a bucket detector and collect all intensity information from the object ͑Refs. 2 and 3͒. Also, for the schematics in Refs. 4 and 14, the object, relative to the source, is positioned in Fresnel region and Fraunhofer region is achieved only in the focal plane of the lens. The schematic of ghost "pinhole" imaging system is shown in Fig. 2͑a͒. Different from previous lensless ghost imaging systems, now the test detector is a single pointlike detector positioned far from the object, and both the object and the reference detector, via free-space propagation of the light field, are located in Fraunhofer region relative to the thermal source. In the experiment, the pseudothermal source S is obtained by illuminating a focused neodym...