Semiconductor laser

Abstract: The disclosed unipolar quantum cascade (QC) laser comprises a multiplicity of essentially identical active regions, with adjacent active regions separated by a superlattice carrier injection/relaxation region (11). A given active region (10) contains a single quantum well (13) with at least two electron states. Lasing is obtained without global intersubband population inversion. Instead, there is believed to exist local population inversion in a small region of k-space near k=0, corresponding to electron energies approximately within an optical phonon energy (∼35meV) from the bottom of the lower subband. A design feature that can be used to improve the thermal characteristics of substantially any QC laser is also disclosed.

Description: Field of the Invention This application pertains to the field of injection semiconductor lasers. Background of the Invention R. F. Kazarinov et al. (Soviet Physics-Semiconductors, Vol. 5(4), p. 707 (1971)) predicted the possibility of amplification of electromagnetic waves in a semiconductor superlattice structure. Since the publication of this seminal paper, the feasibility of a unipolar quantum well semiconductor laser has been considered by many workers in the field. See, for instance, S. J. Borenstain et al., Applied Physics Letters, Vol. 55(7), p. 654 (1989); Q. Hu et al., Applied Physics Letters, Vol. 59(23), p. 2923 (1991); A. Kastalsky et al., Applied Physics Letters, Vol. 59(21), p. 2636 (1991); and W. M. Yee et al., Applied Physics Letters, Vol. 63(8), p. 1089 (1993). However, to the best of our knowledge, the prior art does not disclose observation of lasing in any of the proposed unipolar structures. Known unipolar semiconductor quantum cascade lasers are described in APPLIED PHYSICS LETTERS, vol. 66, no. 5, 30 January 1995, pages 538-540, FAIST J ET AL: "VERTICAL TRANSITION QUANTUM CASCADE LASER WITH BRAGG CONFINED EXCITED STATE"; and ELECTRONICS LETTERS, vol. 30, no. 11, 26 May 1994, page 865/866, FAIST J ET AL: "QUANTUM CASCADE LASER: AN INTERSUB-BAND SEMICONDUCTOR LASER OPERATING ABOVE LIQUID NITROGEN TEMPERATURE". Recently, F. Capasso et al. disclosed a novel unipolar semiconductor laser, designated the quantum cascade (QC) laser See, for instance, U.S. patent No. 5,457,709, issued October 10, 1995 which is related to EP-A-0 676 839 falling under the terms of Article 54(3) EPC. The QC laser comprises a multiplicity of essentially identical undoped "active" regions, a given active region being separated from an adjoining active region by a doped energy relaxation region. According to the exemplary embodiments, each active region comprises two or more coupled quantum wells designed to facilitate attainment of population inversion. The QC laser was exemplarily embodied in the GaInAs/AlInAs system and emits 4.2 µm radiation. In view of the potential importance of lasers of the QC type, it would be highly desirable to have available QC lasers of different structure, in order to give to the device designer greater design freedom. In particular, it would be desirable to have available a QC laser of simpler structure. This application discloses such a QC laser. Summary of the Invention Our study of the physics of QC lasers has lead to the surprising discovery that the presence of two (or possibly more) quantum wells (QWs) in each of the multiplicity of active regions is not an essential requirement, and that a QC laser with a single QW in each of a multiplicity of active regions is feasible. Such a "single QW" laser was made, and lased at the design wavelength of about 4.5 µm. The invention is defined by the claims. More specifically, the invention is embodied in an article that comprises a unipolar semiconductor laser comprising a multilayer semiconductor structure that comprises doped semiconductor material of only a first conductivity type, and further comprising means for applying a voltage across the multilayer semiconductor structure. The multilayer semiconductor structure comprises a multiplicity of essentially identical active regions, a given of said active regions being separated from an adjoining active region by a superlattice carrier injection/relaxation region. Significantly, the given active region comprises a single quantum well. Associated with the single quantum well are a first and a second energy state for charge carriers of the first conductivity type, with the second energy state being higher in energy than the first. The superlattice carrier injection/relaxation region is selected to be relatively transmissive for carriers in the first energy state, and to be substantially less transmissive for carriers in the second energy state. During operation of the laser, at least some of the charge carriers of the first conductivity type undergo a radiative transition from the second to the first energy state. Brief Description of the Drawings FIG.1 schematically depicts a portion of the conduction band diagram of an exemplary single QW laser according to the invention; FIG.2 shows exemplary data on optical power vs. pump current; FIG. 3 shows exemplary spectroscopic and thermal data; and FIG. 4 shows the calculated dispersion of the two subbands of an exemplary single QW QC laser. Detailed Description of Some Preferred Embodiments We will now discuss in greater detail our surprising discovery that a QC laser does not necessarily require two (or more) coupled QWs in each active region but that lasing can be achieved in a QC laser having only one QW in each active region. In the prior art multi-QW QC lasers the relaxation times are selected such that "global" (i.e., integrated over all electron wave numbers) population inversion obtains. We have discovered that attainment of global population inversion is not a necessary condition for lasing, and that laser action, with reasonable threshold, can take place if local population inversion in a small region of k-space near k=0 obtains. The referred-to small region of k-space typically corresponds to electron energies within an optical phonon energy (exemplarily about 35 meV) from the bottom of the lower subband. As will be seen, local population inversion is relatively easily achieved. The general structure of QC lasers according to this invention is substantially like that of the prior art QC laser. See, for instance, Figs. 7 and 10 and associated text of U.S. patent 5,457,709. FIG. 1 schematically shows a portion of the conduction band structure of a single QW laser according to the invention under positive bias (75 kV/cm). Numerals 10 and 11 refer to the active region and the associated Bragg reflector (carrier injector/relaxation) region, respectively, and 12, 13 and 14 refer to first barrier, QW and second barrier, respectively. Shown are also the lower (n=1) and upper (n=2) energy states in the QW, with the respective associated wave functions (moduli squared). The energy difference between the two energy states is approximately 280 meV. The dashed-dotted lines are the effective conduction band edges of the superlattice graded gap electron injector/relaxation regions. Region 15 represents the energy range and spatial extension of band-like electron states, and is referred to as a "miniband". It is separated from upper miniband 16 by "minigap" 17 that substantially blocks electron escape from the upper energy level of the QW. It will be understood that the Bragg reflector superlattice region 11 is designed to result in the minibands and minigap, substantially as described above. The wavy arrow indicates the transition that is responsible for laser action. In an exemplary embodiment of the single QW QC laser, the following Al 0.48 In 0.52 As/Ga 0.47 In 0.53 As layer sequence (starting with injection barrier layer 12 and going from left to right in FIG. 1; thicknesses in nm) was provided: (6.8/4.8), (3.5/2.3), (1.9/2.2), (2.2/2.1), (2.1/2.0), (2.0/1.8), (1.8/1.7), (2.0/1.6), (2.2/1.6), and (2.4/1.4). The layer sequence was not intentionally doped, with the exception of the 14th through 20th layers, which were doped n-type to about 3 x 10 17 cm 3 . The twelfth layer is identified by numeral 18. The exemplary laser structure comprises 25 layer sequences as described. For the lower cladding region of the laser waveguide the n-type InP substrate (~1 - 2 x 10 18 cm -3 ) was used. This results in improved thermal characteristics of the laser, and is considered to be a widely applicable new laser design feature, as will now be discussed. Because of alloy scattering, ternary III/V materials have a thermal resistance that is 15-20 times larger than that of such binary III/V materials as InP or GaAs. For this reason, and to bring the active region of a semiconductor laser closer to the (typically binary) substrate, it is desirable to reduce the thickness of ternary (and/or quaternary) cladding material between the active region and the substrate. Clearly, the absence or substantial reduction of ternary cladding material between the active region and the substrate results in reduced thermal resistance between the active region and the substrate, and consequently in improved thermal characteristics of the laser. We have used this design feature also with multi-QW QC lasers, and believe that it significantly contributed to the attainment of CW operation in these lasers. The feature thus is advantageously used in all types of QC lasers. It will be understood that "substrate" may include a binary III/V buffer layer on the binary bulk III/V material. For the upper cladding region of the exemplary single QW QC laser three AlInAs regions of thickness 700, 600 and 1200 nm, with n-type doping of 1.2 x 10 17 , 3 x 10 17 and 7 x 10 18 cm -3 , respectively, were grown in sequence. Between the waveguide core and the cladding layers were provided 200 nm thick InAs layers, doped n-type to about 1.5 x 10 7 cm -3 , with suitable ~10nm thick interface-smoothing AlInGaAs compositionally graded layers. A top 10 nm thick contact layer (Sn doped to 10 20 cm -3 ), separated from the AlInAs cladding by a 30 nm thick n + AlInGaAs graded layer, completed the growth of the exemplary laser structure. A comparison structure was also grown. Each of the 25 identical active region/Bragg reflector layer sequences of the comparison structure was identical to those of the above described inventive structure, except that the active region contained two QWs, not one. Specifically, the layer sequence of the active region of the comparison structure had the following thicknesses in nm: (6.8/4.8), (2.8/3.9) and (2.7/2.2). All other layers were as described above. Both structures were processed into 2.25 mm long cleaved ridge waveguides of width 11 µm. Current pulses of 50 ns duration were then injected into the devices at 20 kHz repetition rate. FIG. 2 shows peak optical power vs. drive current at 10K of the exemplary single QW QC laser (numeral 21), and of the comparison (2 QW) QC laser (numeral 22). FIG. 3 shows the output spectrum above threshold of the single QW QC laser according to the invention. The inset shows the temperature dependence of the threshold current of the inventive laser. Laser operation of single QW QC lasers will now be discussed with reference to FIG. 4. This discussion is based on our current understanding. It is included for tutorial purposes only, and is not intended to limit the scope of the invention. Lasing in the single QW QC laser is made possible by non-parabolicity of the energy bands, as shown in the energy dispersion relation depicted in FIG. 4, wherein numerals 41 and 42 refer to the energy as a function of momentum parallel to the plane of the QW for, respectively, the n=1 and n=2 states. These non-parabolicities manifest themselves in the different curvature (i.e., different effective mass) of the two states. As a result of this difference in curvature, only electrons that are in a small region of k-space (of width ≲ optical phonon energy, e.g., about 35 meV) near k=0 can absorb photons of energy equal to hv (i.e., the energy difference between the two states at k=0), where ν is the lasing frequency, and h is Planck's constant. The lasing transition is schematically indicated by wavy arrow 43, and dotted arrows 44 and 45 indicate exemplary transitions that can not be excited by the photons of energy hν because the relevant energies differ significantly from hν. In FIG. 4, arrows 46, 471, 472 ... 47N indicate a possible sequence of non-radiative transitions that can result in the transfer of an electron from the n=2 (k ∼ 0) state to the n=1 (k ∼ 0) state. Arrow 46 refers to an inter-subband transition that involves emission of an optical phonon, and arrows 471- 47N refer to intra-subband transitions that also involve emission of optical phonons. The electrons in the n=1, k || > 0 states can tunnel out of the QW at a rate τ-1 tu , and undergo optical phonon scattering at rates τ-1 int,i , where i=1,2 ...... N. Those skilled in the art will recognize that it is necessary that the fraction of electrons in the relevant region near k=0 in the n=1 state is substantially less than 1. Our calculations indicate that this fraction is about 1/2 for the above described single QW QC laser. Those skilled in the art will also recognize that the technique of control of the spatial position of the plasma in the unipolar QC laser by means of a control field that is described in U.S. patent 5,457,709 applies to single QW QC lasers as well as to the prior art multi QW QC lasers, and application of the technique to the former is contemplated.

Claims: An article comprising a unipolar semiconductor laser, said laser comprising a) a multilayer semiconductor structure that comprises doped semiconductor material of only a first conductivity type; and b) means for applying a voltage across said multilayer semiconductor structure; wherein c) said multilayer structure comprises a multiplicity of essentially identical active regions, a given of said active regions (10) being separated from an adjoining active region by a superlattice carrier injection/relaxation region (11); CHARACTERIZED IN THAT d) the given active region comprises a single quantum well (13), associated with said quantum well are only a first n = 1 and a second n = 2 energy state for charge carriers of the first conductivity type, with said second energy state being higher in energy than said first energy state; e) said superlattice carrier injection/relaxation region is selected to be relatively transmissive for carriers in the first energy state n = 1, and to be substantially less transmissive for carriers in the second energy state n = 2; and f) at least some of the charge carriers of the first conductivity type undergo a radiative transition from the second n = 2 to the first n = 1 energy state. Article according to claim 1, wherein the active region is substantially undoped, and the energy relaxation region comprises doped semiconductor material. Article according to claim 1 or claim 2, wherein the energy relaxation region comprises alternating layers of a first and a second semiconductor material. Article according to claim 3, wherein the energy relaxation region comprises a doped superlattice region that comprises a multiplicity of quantum wells. Article according to any of the preceding claims, wherein said multilayer semiconductor structure is selected to provide a waveguide for photons of energy corresponding to said radiative transition. Article according to claim 5, wherein said waveguide cormprises a core that comprises said active region, said core being disposed on a doped binary III/V semiconductor substrate, and further comprises an upper cladding region that comprises doped ternary or quaternary III/V semiconductor material.

Inventors: CAPASSO FEDERICO, CHO ALFRED YI, FAIST JEROME, HUTCHINSON ALBERT LEE, SIRTORI CARLO, SIVCO DEBORAH LEE, CAPASSO, FEDERICO, CHO, ALFRED YI, FAIST, JEROME, HUTCHINSON, ALBERT LEE, SIRTORI, CARLO, SIVCO, DEBORAH LEE
Applicants: AT & T CORP, AT&T IPM CORP.
Application year: 1996
Main classification: H01S5
IPC codes: H01S5, H01L21, H01L33