Steven, no again, and you cannot have read the link to DPReview's article. See page 2, Equivalence of Total Light, and page 4, Real World Total Light Demonstration. It's all there
If I might hazard a guess, you seem to be stuck on the fact that the same subject 'radiates the same amount of light' if I can put it like that, and it doesn't change. What we're discussing is the total amount of light captured by the lens and projected on to the sensor. That does change. A lot.
Sorry, I've been away off-grid...
I've read most things on the topic... and they all seem to convolute things by trying to start from a point of "equivalence" (even that DPreview article, and the example images on pg 4 are particularly poor/misleading IMO).
To really understand it you must start with FOV/scene illuminance. A given area (FOV) can only emit a given amount of light over a given amount of time (it's illuminance)... that cannot be changed, nor can the physics of how light behaves. And that is what we are recording...
Put a 100mm DX lens (if such exists, but it doesn't actually matter) on a 1.5x DX camera and a 150mm FF lens on a FF body. Using the same f(t)-stop on both lenses and from the same distance they will capture the same FOV with the same source illuminance and transmit the same amount of light, and **the exposures will be the same. However, the image circle for the larger sensor is greater than it is for the DX sensor, and that dictates that the light per sq mm is less while the total light (exposure) remains the same (there are more sq mm's recording it).
Everyone seems to get this wrong... exposure (and aperture) is not about "same light per sq mm," as if the light somehow retained the same intensity per each mm as a FOV/scene is spread over a larger image circle... that is impossible. And if a lens could do that, then a lens optimized for a FF sensor would somehow have to increase the total exposure (transmit more light spread over a larger area in order to keep each mm constant), which would necessarily affect it's use/exposure on a crop sensor body. Instead, exposure is about the total light transmitted over the total area/image circle used. I.e. the per in "light per sq mm" means "divided by" and results in the total/overall exposure.
To help understand this we can apply the inverse square law... one way to make an image circle larger is to have a greater distance to the sensor/film plane, and greater distance means less light per sq mm because the image circle is larger. This is in fact what happens with macro/large format photography, it is known as "bellows factor"... in macro photography moving the lens farther away in order to reduce the minimum focus distance increases the size of the image circle and the resulting magnification, and this reduces the amount of light reaching the sensor affecting the exposure (smaller effective aperture). In large format photography it can be either due to actual bellows extension (increased distance/close focusing), or due to using longer FL's for "equivalent/normal" FOV's (spreading a smaller FOV/greater magnification over a larger image circle). The aperture doesn't really have anything to do with the size of the image circle used... it is "constant" only because as you use less of the original/fixed image circle/FOV you are also getting less total light... that is the "same light per square millimeter/less total light" everyone seems to get stuck on, but it has nothing to do with "equivalence" because it does not include the same total scene/FOV/source illuminance.
BTW, bellows factor is the only way to change the size of image circle projected/used while keeping the sensor size constant, but the physics/effect is the same.
From there we have to understand how the inverse square law affects the exposure of a scene/object. If you make a scene/object larger/smaller within the FOV it's exposure (total light) does not change because the light per sq mm changes inversely with size. I.e. if you take a white door and make it larger w/in the FOV it's emitted light per sq mm is reduced, but it occupies more sq mm's and the correct exposure for the door (and the scene overall) remains constant. I.e. the size of an object affects it's "brightness." That's essentially what allows manual exposure to work in a constant light/variable subject/scene situation.
So we have a larger image circle with less light per sq mm -vs- a smaller image circle with more light per sq mm and equivalent total exposures. Next we place the 150mm FF lens on the DX body without changing distance or f(t)-stop. Now the DX sensor is recording a smaller portion of the scene, but it has become "larger" w/in the FOV due to the increased FL. You have less of the scene occupying more of the sensor (what remains is "brighter") and the exposure does not change (assuming even scene illuminance).
And then we can back up 50% of the distance to regain the same/original 100mm FOV which reduces the size of the object(s) w/in the FOV but includes more within it. And again the exposure does not change. And again, that's essentially what allows manual exposure to work in a constant light/variable subject/scene situation. One might think "aha, recording the same FOV from farther w/ DX must mean less light than using the same lens/settings on FF from closer." But it doesn't because the greater distance is offset by the greater concentration/magnification onto the smaller area (same FOV).
All of this is easily tested with a FF camera that has "DX mode" and a constant aperture zoom lens. And all of it is how light/sensors/exposures actually work.
And none of this takes into consideration "DOF equivalence" which would dictate using a larger aperture for the DX sensor. That would increase the amount of light reaching the DX sensor, allowing the use of a lower ISO which offsets the smaller pixel efficiency/sensitivity deficit.
**Complexities arise when you change bodies due to REI/SOS variances/WB handling/flange distances(image circle spread)/sensor characteristics, and when changing lenses due to f vs t stop variances. All of these are typically minor on their own but can combine to create apparent/obvious differences.