In a recent publication, we proposed to apply the resonant tunneling diode (RTD) photodetector principle to the mid-infrared (MIR) spectral region, by combining an antimony-based AlSb/ GaSb double barrier quantum well (DBQW) resonant tunneling structure (RTS) with an narrow bandgap absorption region. [17] Hereby, the RTD serves as an internal high-gain amplifier of small optically generated electrical signals. In contrast to, e.g., avalanche photodiodes where the gain is provided via impact ionization processes, the gain of RTD photodetectors originates from the modulation of a larger majority charge carrier tunneling current that is sensitive to small variations of the local electrostatic potential.The so called 6.1 Å family, [18] which is comprised of the three semiconductors InAs, GaSb, and AlSb offers a huge flexibility in designing electronic, optical, and optoelectronic devices, [19] such as topological insulators, [20][21][22][23] optical MIR type-II superlattice photodetectors, [24] and quantum cascade lasers (QCLs), [25][26][27] or interband cascade lasers (ICLs), [27][28][29][30][31] and interband cascade detectors (ICDs). [32,33] This flexibility can mainly be attributed to the huge variety of band lineups, bandgap energies, and in particular to the so called InAs/GaSb type-II broken bandgap alignment. While the InAs/GaSb/AlSb material system has also brought forth a large variety of different resonant tunneling structures, [3,18,34,35] only AlAsSb/GaSb RTDs provide the required energy barriers in both valence and conduction band due to the type-I heterointerface. [36][37][38][39] In another recent publication, we demonstrated that room temperature resonant tunneling of electrons in AlAsSb/GaSb RTDs requires the use of emitter prewells. [40][41][42] Here, we propose to invert the charge carrier polarity within the RTD photodetector, i.e., using p-type instead of n-type doping.Using p-type doping in an RTD photodetector, and therefore hole instead of electron transport, might seem counterintuitive at first, since hole transport usually comes with several disadvantages. Due to their higher effective mass, holes have a lower mobility and a smaller de Broglie wavelength compared to electrons. [43] A lower mobility results in inferior transport properties, a smaller de Broglie wavelength demands a higher quality semiconductor crystal growth. However, and in particular for the GaSb material system, p-type doping may Mid-infrared (MIR) resonant tunneling diode (RTD) photodetectors based on a p-type doped AlAsSb/GaSb double-barrier quantum well (DBQW) are proposed and investigated for their optoelectronic transport properties. At room temperature, a distinct resonant tunneling current with a region of negative differential conductance is measured. The peak-to-valley current ratio (PVCR) is 1.51. To provide photosensitivity within the MIR spectral region, a lattice-matched quaternary low-bandgap GaInAsSb absorption layer with cutoff wavelength of λ = 2.77 μm is integrated near the DBQW. Under illumination with ...