fig1 is a diagram that illustrates the structure of hybrid electric spacecraft engine 100 in accordance with an illustrative embodiment of the present invention . hybrid electric spacecraft engine 100 comprises plasma containment vessel 110 , plasma generator 120 , laser 130 and electrodes 140 - 1 through 140 - 8 , interrelated as shown . plasma generator 120 is a device for generating a plasma . it is well - known in the art how to make such a device . for example , such a device might comprise a spark generator for generating an electric spark across the face of a solid surface . the heat of the spark causes some of the solid material to vaporize , and then the mobile electrons of the spark ionize the particles of the vaporized material . such ionization results in the vaporized material becoming a plasma comprised of free electrons and free positive ions . for example , the solid material might be made of carbon , in which case the positive ions are carbon atoms that have lost one electron . the mass of one such positive ion is , as is well known in the art , approximately 22 , 000 times as much as the mass of one electron ; but the positive ion has an electric charge that is the same as the charge of one electron , with the opposite sign . plasma containment vessel 110 is a vessel for confining the plasma generated by plasma generator 120 to a finite volume of space . it is well known in the art how to make such a containment vessel . for example , plasma containment vessel might be made of acrylic material . in the illustrative embodiment of the present invention represented in fig1 , plasma containment vessel 110 is made of such material . it will be clear to those skilled in the art , after reading this disclosure , how to make and use plasma containment vessels made of other materials . for example , a class of plasma containment vessels well - known in the art is made not out of ordinary matter , but rather out of magnetic fields . such vessels take advantage of the fact that a plasma is a collection of charged particles whose movements are affected by electric and magnetic fields . of course , such a magnetic vessel requires magnets or magnetic coils made out of ordinary matter for generating the magnetic fields . for example , superconducting coils might be used for such purpose . outlets 150 - 1 and 150 - 2 are openings in one of the walls of plasma containment vessel 110 . they are for allowing some of the plasma particles to escape and , thereby , provide propulsion , as explained in greater detail in the coming paragraphs . in this illustrative embodiment of the present invention , electrodes 140 - 1 through 140 - 8 are wires that are embedded in the wall of plasma containment vessel 110 ; they are placed in the vicinity of openings 150 - 1 and 150 - 2 for the purpose of generating electric fields in and around the openings . they are shown in cross section in fig1 . fig2 depicts a perspective view of plasma containment vessel 110 , as viewed from the outside . the two outlets 150 - 1 and 150 - 2 are visible as openings in the front wall of the vessel , as depicted in the figure . in this depiction , the wires of electrodes 140 - 1 through 140 - 8 are not visible because they are embedded in the acrylic material of which the vessel is made , but they run vertically , as depicted in the figure , along the two openings . it is an important advantage of the present invention that the electrodes are entirely embedded in the acrylic material , such that they never come in contact with plasma particles . therefore , in contrast with ion engines , there is no electric current flowing through electrodes 140 - 1 through 140 - 8 , and they do not experience any damage due to interactions with plasma particles . fig3 is a diagram that illustrates what happens when plasma generator 120 is activated . it is a feature of the present invention that plasma generator 120 is not continuously active . instead , the plasma generator is activated for a short period of time in order to generate a cloud of plasma , depicted in fig3 as plasma cloud 160 , inside plasma containment vessel 110 . in embodiments of the present invention , plasma generator 120 provides enough energy to ionize the plasma , but not much more than that . fig3 also shows that , prior to activating the plasma generator , a voltage is applied to electrodes 140 - 1 through 140 - 8 . in particular , electrodes 140 - 1 , 140 - 2 , 140 - 7 , and 140 - 8 are connected to the positive terminal of a constant - voltage generator , and electrodes 140 - 3 through 140 - 6 are connected to the negative terminal of the constant - voltage generator . such connections are indicated in the figure by “+” or “−” symbols inside the circles that represent the electrodes . the constant - voltage generator is not shown explicitly in fig3 . it is well known in the art how to make a constant - voltage generator . for example , such a generator might be a direct - current ( dc ) power supply that generates a suitable voltage . as already mentioned , it is a feature of the present invention that , nominally , no current flows through electrodes 140 - 1 through 140 - 8 , such that , nominally , the voltage generator does not have to provide any power , just a fixed voltage . in practice , the acrylic material is not a perfect insulator , and some small leakage current is likely to be present . therefore , the dc power supply needs to be kept turned on during normal operation in order to keep the electrodes continually polarized ; however , the amount of energy that the dc power supply must deliver is very small , just enough for counteracting the leakage current . the voltage applied to electrodes 140 - 1 through 140 - 8 results in the creation of electric fields in the volume of space inside outlets 150 - 1 and 150 - 2 . such electric fields are a barrier to the flow of plasma particles , such that the plasma , as generated by the plasma generator , remains inside the containment vessel . this is so because , as noted above , the plasma generator provides only enough energy to ionize the plasma , but not much beyond that . as a result , the kinetic energy of plasma particles is not sufficient for them to overcome the barriers presented by the electric fields in the two outlets . after plasma generator 120 has generated plasma cloud 160 inside plasma containment vessel 110 , laser light is used to accelerate plasma particles . in particular , laser 130 is activated to generate a laser beam . fig4 depicts hybrid electric spacecraft engine 100 with the laser beam illuminating the plasma cloud . the laser beam is depicted as laser beam 170 . the laser beam illuminates a portion of the plasma cloud , such that the plasma particles that are in the path of the beam experience a ponderomotive force . in physics , the ponderomotive force is defined as the force that a charged particle experiences in an inhomogeneous oscillating electric field such as the electric field present in a laser beam . in particular , as the laser light propagates in the laser beam , there is a strong oscillating electric field in the center of the beam . a plasma particle located at or near the center of the beam experiences this oscillating field ; however , the amplitude of the field vanishes if the particle is moved outside of the beam . this decrease in amplitude is an inhomogeneity of the oscillating electric field , and , therefore , plasma particles that are inside the laser beam experience a ponderomotive force that accelerates them in a direction perpendicular to the direction of propagation of the beam . f = - e 2 4 ⁢ m ⁢ ⁢ ω 2 ⁢ ∇ e 2 wherein f is the strength of the ponderomotive force ; e and m are , respectively , the charge and the mass of the charged particle ; ω is the angular frequency of the oscillating field , and e is the peak amplitude of the oscillating electric field . it is important to note that the mass of the charged particle appears in the denominator . therefore , in a plasma wherein electrons are much lighter than positive ions , the effects of the ponderomotive force are felt much more strongly by the electrons than by the positive ions . for example , if the positive ions are carbon ions , the energy acquired by the electrons because of the ponderomotive force is about 22 , 000 times as much as the energy acquired by the ions . in this illustrative embodiment of the present invention , the laser is a pulsed laser ; i . e ., it is a laser that emits light as a sequence of short periodic pulses . each pulse acts on the electrons in the plasma through the ponderomotive force , with negligible effects on the positive ions because of their larger mass . each pulse accelerates the electrons in a direction perpendicular to the direction of propagation of the beam and this acceleration results in an increased kinetic energy of the electrons . as the kinetic energy of the electrons increases after each laser pulse , at some point they will have acquired enough kinetic energy to overcome the barrier presented by the electric fields in outlets 150 - 1 and 150 - 2 . in particular the polarity of the electric fields in outlet 150 - 2 is such that the electrons need less kinetic energy to overcome it , and , therefore , they will start flowing through that outlet as soon as their kinetic energy is large enough . fig5 depicts hybrid electric spacecraft engine 100 with electrons escaping out of the plasma containment vessel through outlet 150 - 2 . the escaping electrons are depicted as electron flow 180 - 1 . outlet 150 - 2 opens into outer space , such that the electrons that escape through the outlet leave the spacecraft entirely . however , electrons are negatively charged , while the positive ions that are left behind are , of course , positively charged . as more and more electrons leave the spacecraft , the spacecraft acquires a positive charge because of the positive ions left behind . therefore , the negative electrons are attracted back toward the spacecraft , and never get too far from it . as more and more electrons accumulate outside the spacecraft , in the volume of space just outside the two outlets 150 - 1 and 150 - 2 , they form a negatively - charged cloud referred to as a “ space charge ”. the presence of the negative space charge on the outside of the containment vessel and in front of the outlets , together with the cloud of positively charged ions that were left behind in the containment vessel , on the other side of the outlets , alters the shape of the electric field in outlet 150 - 1 ; and the attraction of the positive ions by the negative space charge pushes the ions in the direction of the outlet with enough kinetic energy to overcome the barrier in that outlet . much like the polarity of the electric fields in outlet 150 - 2 favored the flow of electrons , the polarity of the electric fields in outlet 150 - 1 favors the flow of positive ions , such that , when the space charge has accumulated enough electrons , positive ions start flowing through outlet 150 - 1 while being accelerated by the electric fields in the outlet . like outlet 150 - 2 , outlet 150 - 1 also opens into outer space , in the same direction as outlet 150 - 2 . therefore , the positive ions that are accelerated by the electric fields in outlet 150 - 1 escape into the same volume of outer space where the space charge is present . there , they recombine with the electrons , and , due to the kinetic energy that they have acquired , they continue moving away from the spacecraft without carrying any electric charge . the electron space charge in this illustrative embodiment of the present invention behaves similarly to the cathode of an ion engine . therefore , it is referred to as a “ virtual cathode ” and is depicted in fig5 as virtual cathode 190 . however , in contrast to an ion engine where the cathode is made out of an electrically conductive material , the space charge is not damaged by the flow of electrons and positive ions . fig6 depicts hybrid electric spacecraft engine 100 with electrons and ions escaping out of the plasma containment vessel through outlets 150 - 1 and 150 - 2 . the escaping ions are depicted as ion flow 180 - 2 . the figure shows that the escaping ions meet the electrons in the space charge , where they recombine and , by virtue of their kinetic energy , continue moving away from the spacecraft , thereby generating thrust through the principle of conservation of momentum . after allowing enough time for a substantial number of positive ions to escape , the process is repeated starting with activation of the plasma generator , as shown in fig3 . fig7 is a flow diagram of a method 700 comprising the salient operations of the process to generate thrust via this illustrative embodiment of the present invention . the figure outlines a number of operations and resultant effects that are interrelated as shown . the hybrid engine in this illustrative embodiment of the present invention executes the outlined operations and directly causes the indicated effects as a result of the recited operations . one or more components of the engine execute one or more of the recited operations , as discussed in more detail above . in regard to method 700 , it will be clear to those having ordinary skill in the art , after reading the present disclosure , how to make and use alternative embodiments of method 700 wherein the recited operations are differently sequenced , grouped , or sub - divided — all within the scope of the present invention . it will be further clear to those skilled in the art , after reading the present disclosure , how to make and use alternative embodiments of method 700 wherein some of the recited operations are optional , are omitted , or are executed by other elements and / or systems associated with the engine ; e . g ., by elements that are external to and interconnected with the ion engine . fig8 shows two possible paths that plasma particles might follow when escaping from plasma containment vessel 110 through outlets 150 - 1 and 150 - 2 . in particular , path 155 - 1 goes from point a to point b to point c , while path 155 - 2 goes from point d to point e to point f . fig9 a is a graph that shows the electrical potential along path 155 - 1 from point a , through point b , to point c . in agreement with the polarity shown in fig3 - 6 , and 8 for electrodes 140 - 1 , 140 - 2 , 140 - 5 , and 140 - 6 , the electric potential first increases and passes through a positive peak , going from a to b , and then decreases and passes through a negative peak , going from b to c . this profile favors the flow of positive ions over negative electrons , as already remarked . the height of the peaks is in proportion to the voltage provided by the constant - voltage generator . the strength of the electric fields associated with the electric potential shown in the figure is in proportion to the height of the peaks and , therefore , the effectiveness of the electric fields as a barrier to the flow of plasma ions can be adjusted as needed by adjusting the voltage provided by the constant - voltage generator . this is an important feature of the present invention , as the ability to adjust the height of the barrier independently of the kinetic energy delivered to the plasma particles , provides additional flexibility in adjusting the thrust generated by the engine . fig9 b is a graph that shows the electrical potential along path 155 - 2 from point d , through point e , to point f . in agreement with the polarity shown in fig3 - 6 , and 8 for electrodes 140 - 3 , 140 - 4 , 140 - 7 , and 140 - 8 , the electric potential first decreases and passes through a negative peak , going from d to e , and then increases and passes through a positive peak , going from e to f . this profile favors the flow of negative electrons over positive ions , as already remarked . similarly to the comment made for fig9 a , the height of the peaks is in proportion to the voltage provided by the constant - voltage and the effectiveness of the electric fields as a barrier to the flow of plasma electrons can be adjusted as needed by adjusting the voltage provided by the constant - voltage generator . fig3 - 6 show one laser 130 for generating laser beam 170 . in some embodiment of the present invention , it is advantageous to use two or more lasers . a second laser can be arranged to generate a second laser beam that propagates in a direction parallel to the direction of laser beam 170 , but in the opposite direction . such a second laser beam is advantageous because second - order effects in the interaction between laser beam 170 and plasma electrons might accelerate the electrons in the direction of the laser beam . such effects are likely to be small , compared to the predominant effect of the ponderomotive force which , as noted above , accelerates the electrons in a direction perpendicular to the direction of propagation of the laser beam . however , in embodiments wherein such second - order effects are undesirable , a second laser arranged as described above can reduce such effects . a second laser is most effective if it generates a laser beam that propagates near laser beam 170 . in particular , it is advantageous if the distance between the two laser beams is , at most , five times the diameter of the larger of the two beams . an important advantage of the present invention over the prior art is that electrons in the plasma are accelerated preferentially over the positive ions , and in a non - random fashion . this is in contrast to the prior - art technique of accelerating all plasma particles by heating the plasma . as noted above , the effect of the ponderomotive force is to accelerate plasma electrons in a direction that is perpendicular to the direction of propagation of the laser beam . such directionality means that , by judiciously positioning the laser beam relative to outlets 150 - 1 and 150 - 2 , it is possible to enhance the proportion of electrons and positive ions that flow through the outlets . the shapes of the two outlets and the position of the laser beam shown in fig4 - 6 have been determined to be advantageous through computer simulations . however , it will be clear to those skilled in the art , after reading this disclosure , how to make and use embodiments of the present invention with other advantageous shapes for any number of outlets and with any number of laser beams advantageously positioned , relative to the outlets , to take advantage of the directionality of the ponderomotive force . it is to be understood that this disclosure teaches just one or more examples of one or more illustrative embodiments , and that many variations of the invention can easily be devised by those skilled in the art after reading this disclosure , and that the scope of the present invention is defined by the claims accompanying this disclosure .