I measured the HiFiMan HE1000s using a G.R.A.S. Model 43AG ear/cheek simulator, a Clio 10 FW audio analyzer, a laptop computer running TrueRTA software with an M-Audio MobilePre USB audio interface, and a Musical Fidelity V-Can headphone amplifier. I moved the headphones around to several different locations on the ear/cheek simulator to find the one that produced the most bass and the most characteristic response. This is a “flat” measurement; no diffuse-field or free-field compensation curve was employed.

This chart shows the HE1000s’ frequency response, which is flat up to 1.5kHz, and rises sharply above that from 2 to 9kHz.

Adding 70 ohms output impedance to the V-Can’s 5 ohms to simulate the effects of using a typical low-quality headphone amp has no audible effect on the HE1000s’ frequency response.

This chart compares the HE1000s (blue trace) with HiFiMan’s HE560s (red trace) and Audeze’s LCD-3s (green trace). The HE1000s have a similar response to the HE560s, with about 5dB more energy between 5 and 9kHz, and a little more bass to help balance out that treble peak. The LCD-3s have much less treble energy above 2.5kHz, and a flatter measured response, than either HiFiMan model. Note that, unlike with most speakers, a flat measured response in headphones does not necessarily equate with a flat perceived response.

The HE1000s’ waterfall plot may not look very clean at first glance, but if you look close you’ll see that all those little blue streaks are resonances of very narrow bandwidth about -40dB below the test signal. The only resonance shown here that might be audible is the combination of two adjacent -20dB resonances near 5kHz.

The total harmonic distortion (THD) of the HE1000s is well below audible levels, even at the extremely high level of 100dBA, measured with pink noise.

In this chart, the external noise level is 75dB SPL; the numbers below that indicate attenuation of outside sounds. As is almost always the case with open-back headphones, the HiFiMan HE1000s provide essentially no noise isolation; any sounds from outside them will come right through.

The impedance magnitude of the HE1000s is nearly dead flat at 37 ohms; the impedance phase, too, is nearly flat.
The sensitivity of the HE1000s, measured between 300Hz and 3kHz with a 1mW signal calculated for the specified impedance of 35 ohms, is 88.1dB. Although that’s relatively low, as I say in the review, it was enough for me to get a fairly comfortable volume level from my smartphone.
. . . Brent Butterworth
brentb@soundstagenetwork.com
I measured the NightHawks using a G.R.A.S. Model 43AG ear/cheek simulator, a Clio 10 FW audio analyzer, a laptop computer running TrueRTA software with an M-Audio MobilePre USB audio interface, and a Musical Fidelity V-Can headphone amplifier. I moved the NightHawk earpiece around to several different locations on the ear/cheek simulator to find the position that gave the most bass and the best average of midrange and treble responses. This is a “flat” measurement; no diffuse-field or free-field compensation curve was employed.

This chart shows the NightHawks’ frequency response, which is most notable for being fairly flat, with little to none of the usual peak between 2 and 4kHz. There’s a dip centered at 1.2kHz, and a gradual bass rolloff.

Adding 70 ohms of output impedance to the V-Can’s 5 ohms to simulate the effects of using a typical low-quality headphone amp has no audible effect on the NightHawks’ frequency response.

This chart compares the NightHawks (blue trace) with the Oppo Digital PM-3s (red trace) and the NAD Viso HP50s (green trace); both of the latter have received generally positive reviews. The NightHawks are clearly very different, with a more resonant (less flat) bass response and about 10dB less treble energy on average.

The NightHawks’ waterfall plot looks clean, with no major resonances, and very low resonance in the bass frequencies compared with most over-ear headphones I’ve measured.

The total harmonic distortion (THD) of the NightHawks is, as claimed by AQ, very low, even at the extremely high level of 100dBA, measured with pink noise. Even at 10Hz/100dB, there is only 1% THD. Note that because of the AQs’ semi-open-back design and the fact that I measure distortion in a very quiet room but not in an anechoic chamber, even the slight distortion seen in this chart may be mostly noise leaking in. (To improve the signal/noise ratio of this measurement, I use denim insulation on the back of open-back and semi-open-back headphones, but it’s not perfect.)

In this chart, the external noise level is 75dB SPL; the numbers below that indicate the degree of attenuation of outside sounds. The NightHawks’ isolation is roughly what I’ve measured from typical closed-back designs -- remarkable for a semi-open-back model. Consider AudioQuest’s claims for their diffuser confirmed.

The impedance magnitude of the NightHawks is basically flat, but my test gear measured it as 13 ohms -- much less than the specified 25 ohms. (I checked the test setup with a couple of other headphones; it was working properly.) The impedance phase, too, is basically flat.
The NightHawks’ sensitivity, measured between 300Hz and 3kHz with a 1mW signal calculated for the claimed 25-ohm impedance, averages 100.4dB -- enough to get plenty of volume from almost any source device.
. . . Brent Butterworth
brentb@soundstagenetwork.com
I measured the PSB M4U 4s using a G.R.A.S. Model RA0045 ear simulator, a Clio 10 FW audio analyzer, a laptop computer running TrueRTA software with an M-Audio MobilePre USB audio interface, and a Musical Fidelity V-Can headphone amplifier. I used one of the supplied Comply foam eartips because that’s what designer Paul Barton used when voicing this model. For comparison, I also include a measurement taken with one of the supplied silicone eartips. This is a “flat” measurement; no diffuse-field or free-field compensation curve was employed.

Here is the frequency response of the M4U 4s using a supplied Comply foam eartip. It’s fairly similar to the responses we measure with most high-quality earphones, the only aspects of note being a little more energy than usual around 1.5kHz, and a little less than usual from 8 to 10kHz.
![]()
This chart shows the M4U 4s’ frequency response with the Comply foam eartip (red trace), and with the smallest of the supplied silicone tips (purple trace). The silicone tip causes a boost of 2-3dB in upper-midrange/lower-treble energy, a deep dip at 7kHz, and a 3-10dB increase in output between 8 and 12kHz. PSB’s silicone eartips will likely sound significantly brighter.

Adding 70 ohms of output impedance to the V-Can’s 5 ohms to simulate the effects of using a typical low-quality headphone amp has only a very slight effect on the M4U 4s, boosting the bass by 0.8dB at 20Hz (this will be inaudible), and reducing the output between 2 and 3kHz by 0.5-1dB (might be barely audible). Most balanced-armatures headphone show a much bigger and more significant frequency-response swing in this test.

You can see from this chart that the M4U 4s (blue trace) have more bass and treble output than do NAD’s Viso HP20 earphones (green trace), also designed by Paul Barton, or Sony’s XBA-H1s (red trace), a well-regarded hybrid design.

Other than the bass resonances seen in almost every spectral-decay measurement of headphones, the M4U 4s are essentially resonance-free.

The M4U 4s’ total harmonic distortion (THD) is very low, with just a couple of slight, narrow peaks at 1 and 4kHz, where the THD rises to 2.5-5% -- and that’s only at the extremely loud level of 100dBA, measured with pink noise.

In this chart, the sound-pressure level (SPL) of external noise is 75dB; the numbers below that indicate the degree of attenuation of external sounds. With either the Comply (green trace) or the silicone (purple trace) eartips, the M4U 4s’ isolation is outstanding for passive earphones. In fact, I had to expand this chart’s Y axis to accommodate the traces; normally, the lowest number along the Y axis is 30dB.

Here’s why, unlike with almost all other headphones using balanced-armature drivers, the M4U 4s’ response doesn’t really change when the user switches to a high-impedance source device. The impedances of most balanced-armature ’phones increase radically at high frequencies, but the M4U 4s’ impedance remains between 18 and 22 ohms throughout the audioband.
The M4U 4s’ sensitivity, measured from 300Hz to 3kHz with a 1mW signal calculated for the claimed 16-ohm impedance, is 99.7dB. Technically, that’s a little lower than average for earphones, but it’s plenty high enough to get a satisfying volume level from any portable device.
. . . Brent Butterworth
brentb@soundstagenetwork.com
I measured the Bowers & Wilkins P5 Series 2s using a G.R.A.S. Model 43AG ear/cheek simulator, a Clio 10 FW audio analyzer, a laptop computer running TrueRTA software with an M-Audio MobilePre USB audio interface, and a Musical Fidelity V-Can headphone amplifier. I moved the headphones around to several different locations on the ear/cheek simulator to find the spot that gave the most bass and the most characteristic response. As I usually do with on-ear headphones, I used the ear/cheek simulator’s clamping mechanism to ensure a good seal. This is a “flat” measurement; no diffuse-field or free-field compensation curve was employed.

This chart shows the P5 Series 2s’ frequency response. Its obvious distinguishing characteristic is the big dip in the midrange, centered at 500Hz. That peak, centered at 2.3kHz, is broad and high in amplitude, leading me to speculate that many listeners will find the P5s to sound a little bright. You may notice the disparity in bass response between the left (blue) and right (red) channels. That’s the best bass output I could get from the left channel after repeated repositionings of the earpiece, but keep in mind that the acoustical mating of the ear/cheek simulator to on-ear models is too fussy and unpredictable for me to take off points here.

Adding 70 ohms output impedance to the V-Can’s 5 ohms to simulate the effects of using a typical low-quality headphone amp has little effect on the P5 Series 2s other than a boost in the bass of about 1dB below 80Hz.

This chart compares the P5 Series 2 with a well-regarded on-ear model, Beyerdynamic’s T51p (red trace), as well as my reference headphones for the $300 price point: NAD’s Viso HP50s (green trace). These are normalized to 94dB at 500Hz, per my standard practice for headphone frequency-response measurements and as mandated by the IEC’s 60268-7 standard, which makes it look as if the P5 Series 2s have a lot more bass and treble output than the other headphones -- but it’s more accurate to think of them as having a huge midrange dip around 500Hz.

The P5 Series 2s’ waterfall plot looks very clean, with no noteworthy resonances.

The total harmonic distortion (THD) of the P5 Series 2s is typical for on-ear ’phones. At the loud listening level of 90dBA (measured with pink noise), the THD rises to 2% at 20Hz, which you’re very unlikely to notice (unless you often listen to Saint-Saëns’s “Organ Symphony”). At the very loud listening level of 100dBA, the THD runs about 4.5% below 40Hz.

In this chart, the external noise level is 75dB SPL; the numbers below that indicate the degree of attenuation of outside sounds. With very little reduction of level in sounds below 1kHz, and none in the “jet engine band” of about 50-100Hz, this is typical performance for passive on-ear headphones.

The impedance of the P5 Series 2s is mostly flat, staying between 24 and 30 ohms through the entire audioband.
The sensitivity of the P5 Series 2s, measured between 300Hz and 3kHz with a 1mW signal calculated for the rated 22 ohms impedance, is 101.2dB. This is typical for on-ear headphones.
. . . Brent Butterworth
brentb@soundstagenetwork.com
I measured the Oppo PM-3s using a G.R.A.S. Model 43AG ear/cheek simulator, a Clio 10 FW audio analyzer, a laptop computer running TrueRTA software with an M-Audio MobilePre USB audio interface, and a Musical Fidelity V-Can headphone amplifier. Measurements were calibrated for ear reference point (ERP), roughly the point in space where the center axis of your eardrum would intersect with your palm if you pressed your hand against your earlobe. I moved the headphones around to several different locations on the ear/cheek simulator to find the one that produced the most bass and the most characteristic response. This is a “flat” measurement; no diffuse-field or free-field compensation curve was employed.

This chart shows the PM-3s’ frequency response, which is just a little bit atypical in that the usual peak centered somewhere near 3kHz is more like a hill. So it’s a broader boost than usual, and the peak around 7.5kHz is a little stronger than usual. Thus, this measurement suggests a fairly neutral tonal balance but a somewhat unusual sound.

Adding 70 ohms of output impedance to the V-Can’s 5 ohms, to simulate a typical low-quality headphone amp, has essentially zero effect on the PM-3s’ frequency response.

This chart compares the closed-back PM-3s (blue trace) with Oppo’s open-back PM-2s (red trace) and NAD’s closed-back Viso HP50s (green trace). The PM-2s and HP50s obviously have flatter responses; the PM-3s are likely to be perceived as sounding more trebly than either.

The PM-3s’ waterfall plot is pretty clean, with much less bass resonance than the norm. The only noteworthy resonances in the mids and treble are centered at 2.1 and 3kHz. They’re well damped, though, and die out after about 8ms.

The Oppos’ total harmonic distortion (THD) is practically nonexistent. This is one of the lowest distortion figures I have measured in a set of headphones.

In this chart, the level of external noise is 75dB SPL; the numbers below that indicate the degree of attenuation of outside sounds. This result is very good for over-ear (i.e., circumaural), passive headphones, with reductions of 10dB at 1kHz, and as much as 35dB at higher frequencies. However, it won’t have much effect on jet-engine noise, which is typically loudest between 50 and 200Hz.

The PM-3s’ impedance magnitude and phase are almost dead flat at 26 ohms -- the same as Oppo’s spec.
The sensitivity of the PM-3s, measured between 300Hz and 3kHz with a 1mW signal and calculated for the specified impedance of 26 ohms, is 99.8dB -- enough to get decent volume levels from most portable devices.
. . . Brent Butterworth
brentb@soundstagenetwork.com
I measured the Torque t402v headphones using a G.R.A.S. Model 43AG ear/cheek simulator, a Clio 10 FW audio analyzer, a laptop computer running TrueRTA software with an M-Audio MobilePre USB audio interface, and a Musical Fidelity V-Can headphone amplifier. Measurements were calibrated for ear reference point (ERP), roughly the point in space where the center axis of your eardrum would intersect with your palm if you pressed your hand against your earlobe. I moved the headphones around to several different locations on the ear/cheek simulator to find the one with the most bass and the most characteristic response. In measurements of the headphones with the on-ear earpad, I used the G.R.A.S. 43AG’s clamping mechanism to ensure a good seal. This was a “flat” measurement; no diffuse-field or free-field compensation curve was employed.

This chart shows the t402v’s frequency response with the over-ear pad in the four different sound modes. The traces are color-coded to the modes: yellow for yellow mode, blue for blue mode, etc. With all modes, there’s a fairly large midrange dip between 400Hz and 1.5kHz, and the peak between 5kHz and 8kHz is stronger than the peak at 3kHz. With most headphones, the 3kHz peak is stronger. Yellow mode measured as being a lot more bassy than the other modes.

This chart shows the frequency response with the on-ear pad, again color-coded by mode. This is a much more typical response than I measured with the over-ear pad, with a mild midrange dip centered at 750Hz and a moderate (for headphones) peak at 3kHz. The magnitude of the measured differences among the modes was less with the on-ear pad.

Adding 70 ohms to the V-Can’s 5-ohm output impedance to simulate the effects of using a typical low-quality headphone amp had little effect on the t402v. This result is normalized at 1kHz, per my standard procedure. A tiny peak in the impedance produced a slight and probably inaudible boost centered at 1.1kHz, but otherwise the impedance change in the source had no effect on the frequency response.

This chart compares the t402v with on-ear pad in black mode (dark blue trace) and over-ear pad in black mode (light blue) with NAD’s Viso HP50 over-ear model (red) and Beyerdynamic’s tunable Custom One Pro with its tuning level in position 2 “linear” (green). The HP50 obviously had the flattest response of the three; in on-ear and over-ear modes, the t402v was bassier than the other two.

The t402v’s waterfall plot is very clean, with much less resonance than I usually see in headphones of this type. You can see a mild resonance at that impedance peak centered at 1.1kHz, but because it’s well damped, it dies out almost immediately. The measurement shown was taken with the over-ear pad; the result with the on-ear pad was even cleaner.

The t402v’s total harmonic distortion (THD) was moderate with the on-ear pad, but higher with the over-ear pad because of the headphone’s lower sensitivity with the latter pad. In the above chart, results with the on-ear pad are shown in the dark traces, at 90dBA (dark green) and 100dBA (dark orange); results with the over-ear pad are shown in the light traces, at 90dBA (light green) and 100dBA (light orange). With the on-ear pad, the THD is fairly typical: at 90dBA, 1% at 100Hz and 3% at 20Hz, those numbers respectively rising to 2% and 7% at the very loud listening level of 100dBA. With the over-ear pad, the results at 90dBA (still quite a loud level) were similar to the 100dBA results with the on-ear pad, but at 100dBA the distortion was pretty high. However, it’s unlikely that you could reach such high levels with the over-ear pads installed if you’re driving these headphones with a phone or tablet.

In this chart, the level of external noise is 75dB SPL; the numbers below that indicate the attenuation of outside sounds. The green trace shows the t402v’s isolation with the on-ear pad, the purple trace the result with the over-ear pad. These results are typical for passive on-ear and over-ear headphones; you’ll get very little reduction of level in sounds below 1kHz.

The t402v’s impedance is essentially flat, averaging 18 ohms, with very moderate phase shift. As noted above, the Torque’s impedance does have a slight peak centered at 1.1kHz.
The sensitivity of the t402v, measured between 300Hz and 3kHz with a 1mW signal and calculated for the rated 16-ohm impedance in black mode, was 101.6dB with the on-ear pad and 93.9dB with the over-ear pad. The on-ear results are typical for closed-back headphones, but the over-ear results are low -- more like what I’d expect to measure from audiophile-oriented planar-magnetic headphones.
. . . Brent Butterworth
brentb@soundstagenetwork.com
I measured the Phiaton MS 100 BAs using a G.R.A.S. Model RA0045 ear simulator, a Clio 10 FW audio analyzer, a laptop computer running TrueRTA software with an M-Audio MobilePre USB audio interface, and a Musical Fidelity V-Can headphone amplifier. Measurements were calibrated for drum reference point (DRP), roughly the point at the center of the eardrum (in this case, the center of the measurement mike). I used the Phiatons’ medium-size eartips because those best fit the RA0045. This is a “flat” measurement; no diffuse-field or free-field compensation curve was employed.

This chart shows the frequency response of the MS 100 BAs. It’s surprisingly flat -- most earphones have a larger dip in the midrange and a bigger bump in the bass -- which suggests that the Phiatons may sound smoother, but less vivid and less exciting, than many of their competitors.

As with most headphones using balanced-armature drivers, adding 70 ohms output impedance to the V-Can’s 5 ohms, to simulate the effects of using a typical low-quality headphone amp, has a large effect on the MS 100 BAs’ tonal balance. If you connect it to a high-quality source device, it has a flat response; if you connect it to a high-impedance source device (such as the headphone amps built into most laptops), the treble will be boosted a couple dB and the bass reduced by about 5dB -- easily audible differences.

The MS 100 BAs’ departure from the norm is visible in this comparison with NAD’s HP20 dynamic earphones and Sony’s XBA-H1 hybrid dynamic/balanced-armature earphones. The midrange dip visible in the NADs’ and Sonys’ responses is usually thought to produce a subjectively flatter response and a more spacious sound. However, the science here is still developing.

The Phiaton MS 100 BAs show no significant resonances above 800Hz, which is excellent performance.

The MS 100 BAs’ total harmonic distortion (THD) is relatively high; at 100Hz, it’s 2% at 90dBA and 7.5% at 100dBA. Competitors such as the Marshall Mode EQs post numbers more in the range of 1-2%. However, note that 100dBA (level measured with pink noise) is an extremely high listening level; I include it here mainly because some headphones can handle it and some can’t. Also note that research has shown that headphone distortion is rarely audible except when it’s very high.

In this chart, the external noise is at an SPL of 75dB; the numbers below that indicate the Phiatons’ attenuation of outside sounds. Their isolation is very good for earphones, reducing noise by 20dB at 100Hz (the middle of the “airplane cabin-noise band”) and by up to 32dB in the treble. Note that your results may not be as good, depending on the size and shape of your ear canals and on the size of eartips you choose.

This is the biggest impedance swing I can remember measuring in a passive headphone model: from 24 ohms in the bass to about 460 ohms at 20kHz. This is why the Phiatons’ tonal response changes so much when they’re used with a high-impedance source device.
The Phiatons’ sensitivity, measured between 300Hz and 3kHz with a 1mW signal and calculated for the rated 24 ohms impedance, is 110.8dB, which is exceptionally high. This means that the MS 100 BAs will be able to deliver high playback levels from practically any source device.
. . . Brent Butterworth
brentb@soundstagenetwork.com
I measured the Marshall Mode EQs using a G.R.A.S. Model RA0045 ear simulator, a Clio 10 FW audio analyzer, a laptop computer running TrueRTA software with an M-Audio MobilePre USB audio interface, and a Musical Fidelity V-Can headphone amplifier. Measurements were calibrated for drum reference point (DRP), roughly the point at the center of your eardrum (in this case, the center of the measurement microphone). I used the medium-sized eartips because those best fit the RA0045. This is a “flat” measurement; no diffuse-field or freefield compensation curve was employed.

This is the frequency response of the Mode EQs in EQ1 mode. (The comparison with EQ2 mode is shown below.) This measurement may look very uneven, but it’s actually a fairly common response for earphones. The bass boost and the midrange peak at 2.5kHz are intended to compensate for the fact that the earphones effectively bypass the acoustical effects of the earlobes and ear canals.

This chart shows the Mode EQs’ frequency response in EQ1 and EQ2 modes. The response is effectively the same, except that EQ2 mode reduces bass by about 3dB.

Adding 70 ohms to the V-Can’s output impedance of 5 ohms, to simulate the effects of using a typical low-quality headphone amp, has a modest effect on the Mode EQs in EQ1 mode (shown here), but a much larger effect in EQ2. In EQ1, the higher-impedance source shows a bass boost of about 0.5dB and, beginning above 2.5kHz, a treble rolloff of about 2dB. In EQ2, though, using a low-quality amp (like the ones built into most Windows laptops and some cheap smartphones) will soften the sound significantly, boosting bass by about 2dB and, starting at about 1.5kHz, reducing the treble by a like amount.

You can see from this chart that the Mode EQs (shown here in EQ1 mode) have a more extreme bass boost and a more extreme upper-midrange/lower-treble peak than the NAD HP20s or the Sony XBA-H1s, both of which produce comparatively neutral sounds.

The Mode EQs’ spectral decay plot shows some unusual and very narrow resonances at 6, 8, and 12kHz, and a little more bass resonance than is usual for dynamic earphones, but there’s nothing particularly troubling here.

The total harmonic distortion (THD) of the Mode EQs in EQ1 mode is insignificant, showing a slight rise around 800Hz but never rising even to 2% at the very high listening level of 100dBA.

In this chart, the sound-pressure level (SPL) of external noise is 75dB; the numbers below that indicate attenuation of outside sounds. The Mode EQs’ isolation is perhaps a little better than average for earphones, with a reduction of 10 to 30dB through most of the audioband. Note that, depending on the size and shape of your ear canals and on the eartips you choose, your results may not be as good.

Here’s why the response in EQ2 mode changes a lot depending on the output impedance of the source device. The impedance swing in EQ2 is huge for earphones with dynamic drivers, dropping from 49 ohms in the bass to 17 ohms in the treble. It’s much less extreme in EQ1 mode, which has a maximum impedance of 31 ohms. I assume that the extreme impedance shift in EQ2 mode is due to the filter used in the EQ switch.
The Mode EQs’ sensitivity, measured between 300Hz and 3kHz with a 1mW signal calculated for the rated 30 ohms impedance, is 108.1dB in EQ1 mode, 107.0dB in EQ2 mode -- sensitive enough to get loud levels from practically any source device.
. . . Brent Butterworth
brentb@soundstagenetwork.com
The following categories containing listings of all product reviews published by the SoundStage! Network since 1995 from all of our online publications. The products are divided into categories and listed in descending order by date. There is no Search function within the listings, but you can search by bringing up the page with the appropriate list and using the "Find" command on your browser. (For Internet Explorer select: Edit > Find on this Page.)