This is Rigol's
probes characteristics table:

According to
Rigol's RP2200 specifications, the DS1052E's probes are rated to 150MHz and 300VAC when set x10 and to 7MHz and 150VAC when set x1.
The oscilloscope probes are extremely complicated animals, despite the textbooks that describe them as simple passive devices with resistive and capacitive dividers. For example, no x1 passive probe can go further beyond the 20..50 MHz barrier. Why?
Please, read an excellent article by Doug Ford on the oscilloscope probes, that was published at the Silicon Chip in 2009:
The secret world of Oscilloscope Probes.
I barely use Rigol's probes, since I have better results using much better ones (x100/250MHz). Just watch the table below, to see what a difference can a better probe make. By the way, I use the fragile RP2200's only when the signal is very low in amplitude to be measured by the x100 probes.
Now, this is an eloquent example of
probe loading, while reading the crystal oscillator output pin ("TOSC2") of an Atmel ATmega8 μC running at 16MHz:
ATmega8: Vcc = 5.04V, DDS disconnected, CKOPT fuse enabled:
TOSC2: 4.76Vpp, loaded with a x100 probe (100MΩ//6.5pF)
TOSC2: 4.48Vpp, loaded with a x10 probe (10MΩ//17pF)
TOSC2: 3.56Vpp, loaded with two x10 probes
ATmega8: Vcc = 5.04V, DDS disconnected, CKOPT fuse disabled:
TOSC2: 582mVpp, loaded with a x100 probe
TOSC2: 312mVpp, loaded with a x10 probe
TOSC2: 184mVpp, loaded with two x10 probes
The "CKOPT fuse" controls the xtal oscillator output swing amplitude and, in consequence, the oscillator's power consumption and fan-out.
P.S. I did not even bother to make any measurements of TOSC2 with the probes set x1 (1MΩ//100pF)...
By the way, "No probes are made equal"!
-George