Given that rockets are clearly not cut for this, I find it rather weird that, despite a couple mentions in the comments, Breakthrough Starshot isn't getting more discussion here even though it was literally the first thing that came to my mind when I saw this question up. And that leads one to naturally consider the state of the art of beam propulsion, for that is what is relevant here.
Beamed propulsion, of course, circumvents the rocket equation by leaving the fuel on the ground, so that the "have to lift fuel to lift fuel to lift fuel to ..." business that creates the exponential problem with rockets no longer applies.
Now, the simplest method to do beamed propulsion, perhaps, is a laser and, indeed, BTSS aimed to use exactly such. Given that BTSS is not expected to produce results for some 50 years or more (iirc), then I'd say this isn't "present day" by your definition but, given that posts have at least examined the feasibility of using existing rockets, I find it is only fair to try a similar at least cursory analysis of the existing possibilities for laser beam propulsion.
Beam propulsion, of course, works on the principle that light carries momentum as well as energy and, so, if suitably directed at a craft, can create a force (transfer of momentum) upon it. The relevant equation is Einstein's
$$p = \frac{E}{c}$$
where $E$ is the energy in the beam of light. If the spacecraft is an ideal reflector, it will manage to acquire twice this much because the beam is reflected back, and that back-reflection must be balanced by an extra forward momentum equal to the whole original beam thanks to the conservation of momentum.
Note, of course, that there is the factor $c$ in the denominator, which, in human scale units, is crazy big: as a result, even a modest energy will only produce a little extra momentum and, hence, only minimal acceleration of a spacecraft. In particular, using $p = \gamma mv$ for a general relativistic spacecraft, we see the energy required to accelerate to speed $v$ is
$$E_\mathrm{accel} = \frac{\gamma mc v}{2}$$
for the ideal-reflection case. Likewise, if we are alloted a certain amount of energy and want a certain goal speed, we can figure the maximum mass:
$$m_\mathrm{max} = \frac{2E}{c\gamma v}$$
So how much laser energy can we reasonably muster? Well, there apparently was one laser from as far back as the 1980s called "MIRACL", which was a chemical gasdynamic laser meaning that instead of electric power it was fueled directly by a special chemical fuel and obtained a peak power exceeding 1 MW and 70 s firing time, which means you can have 70 MJ to play with.
Since it has been built, it could be again and, perhaps better now. Thus I'd say - while I don't know if this is the state of the art now - it could definitely be a reasonable value for "today". Suppose we build 100 of these lasers - that would be 7000 MJ, and we want to figure out the largest mass. Using speed $0.1\ \mathrm{c}$, so that $\gamma \approx 1.005$ and
$$m_\mathrm{max} = \frac{2(7000\ \mathrm{MJ})}{(3.00 \times 10^8\ \mathrm{m/s})^2 \cdot 1.005 \cdot 0.1} \approx 1.54 \times 10^{-12}\ \mathrm{MJ \cdot {s^2/m^2}}$$
or $1.54 \times 10^{-12}\ \mathrm{Gg}$ (gigagrams). Taking those units down we see this is about 1.5 milligrams.
The question then becomes whether you can do anything useful with 1.5 mg of total payload, most of which will have to be taken up by the light sail - indeed, if such a light sail is possible at all. Hence whether this qualifies as "a probe" is something for which I would exercise considerable caution and mind you that I am much more of a theoretician than an engineer, so those who are more savvy with the latter may want to chime in and complete this answer. Moreover, note that this has some very optimistic hidden assumptions such as that we can reflect 100% of the laser light (impossible), and that we can keep 100% of the beam focused on the craft (this is a big issue with the real BTSS project). Hence maybe you could say that 0.15 mg might be a better target and, it doesn't then start to sound too good for the sail.
One can, of course, work the other way, too: given the energy and a craft mass, how fast can we get it? $0.1\ \mathrm{c}$ may be out, but what about if we're willing to at least send an interstellar precursor, e.g. something like the "thousand astronomical units" (TAU) that was once upon a time proposed a very long time ago. Suppose we were to take a craft mass of, say, 1 gram, or 1000 mg. Using the same equations, we can solve for $\gamma v$ by
$$\gamma v = \frac{2E}{mc}$$
so that with now $E = 7000\ \mathrm{MJ}$ and $m = 10^{-9}\ \mathrm{Gg}$, we get a $\gamma v$ of about $46\ \mathrm{km/s}$, so this is about the actual velocity. Not much better than chemical rockets, but could get you to 1000 AU - 150 000 Gm - in (noting that km/s is the same as Gm/Ms) ~3200 Ms which, while longer than a typical human lifetime of 2200 Ms (~70 years) or even a long one of 3000, is still within range of a few who'd be lucky. Still rather abysmal though esp. given what I said about this being very idealized as in the previous case.
So I'd say that, yeah, it is probably not feasible to get a space probe going with this route either. Nonetheless, I'm at least a little surprised by how and that is actually something you could perhaps at least see with your eyes that we just might, were we to deem it worthy of spending the money, loft, if not right now then quite sooner than 50 years (1577Ms). Keep in mind that "cool" can, if nothing else, be inspiration for better.
One more angle I'd point out is that in order for the lasers to be really useful, you'd ideally not want to launch this from Earth, but rather from the Moon, because of the atmosphere. Fortunately, a chemical gasdynamic laser is near-ideal for that due to the fact that it contains its own powerplant; the downside is MIRACL was a pretty big thing, and would require a lot of launch capacity to get 100 of them to the Moon. Nonetheless, it could be possible esp. with Elon Musk's BFRs - though that still is "not today".