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  • 參數(shù)資料
    型號: ADF4153WYRUZ-RL7
    廠商: Analog Devices Inc
    文件頁數(shù): 11/24頁
    文件大小: 0K
    描述: IC SYNTH PLL RF F-N FREQ 16TSSOP
    標準包裝: 1
    類型: 分數(shù) N 合成器(RF)
    PLL:
    輸入: CMOS
    輸出: 時鐘
    電路數(shù): 1
    比率 - 輸入:輸出: 2:1
    差分 - 輸入:輸出: 是/無
    頻率 - 最大: 4GHz
    除法器/乘法器: 無/是
    電源電壓: 2.7 V ~ 3.3 V
    工作溫度: -40°C ~ 125°C
    安裝類型: 表面貼裝
    封裝/外殼: 16-TSSOP(0.173",4.40mm 寬)
    供應商設備封裝: 16-TSSOP
    包裝: 標準包裝
    其它名稱: ADF4153WYRUZ-RL7DKR
    Data Sheet
    ADF4153
    Rev. F | Page 19 of 24
    The programmable modulus is also very useful for multi-
    standard applications. If a dual-mode phone requires PDC
    and GSM 1800 standards, the programmable modulus is of
    great benefit. PDC requires 25 kHz channel step resolution,
    whereas GSM 1800 requires 200 kHz channel step resolution.
    A 13 MHz reference signal can be fed directly to the PFD.
    The modulus is programmed to 520 when in PDC mode
    (13 MHz/520 = 25 kHz). The modulus is reprogrammed to
    65for GSM 1800 operation (13 MHz/65 = 200 kHz). It is
    important that the PFD frequency remains constant (13 MHz).
    This allows the user to design one loop filter that can be used in
    both setups without running into stability issues. It is the ratio
    of the RF frequency to the PFD frequency that affects the loop
    design. By keeping this relationship constant, the same loop
    filter can be used in both applications.
    FASTLOCK WITH SPURIOUS OPTIMIZATION
    As mentioned in the Noise and Spur Mode section, the part can
    be optimized for spurious performance. However, in fastlocking
    applications, the loop bandwidth needs to be wide, and
    therefore the filter does not provide much attenuation of the
    spurs. The programmable charge pump can be used to get
    around this issue. The filter is designed for a narrow-loop
    bandwidth so that steady-state spurious specifications are met.
    This is designed using the lowest charge pump current setting.
    To implement fastlock during a frequency jump, the charge
    pump current is set to the maximum setting for the duration of
    the jump by asserting the fastlock bit in the N divider register.
    This widens the loop bandwidth, which improves lock time. To
    maintain loop stability while in wide bandwidth mode, the loop
    filter needs to be modified. This is achieved by switching in a
    resistor (R1A) in parallel with the damping resistor in the loop
    filter (see Figure 16). MUXOUT needs to be set to the fastlock
    switch to use the internal switch. For example, if the charge
    pump current is increased by 16, the damping resistor, R1,
    needs to be decreased by while in wide bandwidth mode.
    ADF4153
    VCO
    C2
    C1
    CP
    FL
    MUXOUT
    R1
    R1A
    03685-
    029
    Figure 16. ADF4153 with Fastlock
    The value of R1A is then chosen so that the total parallel
    resistance of R1 and R1A equals 1/4 of R1 alone. This gives
    an overall 4× increase in loop bandwidth, while maintaining
    stability in wide bandwidth mode.
    When the PLL has locked to the new frequency, the charge
    pump is again programmed to the lowest charge pump current
    setting by setting the fastlock bit to 0. The internal switch opens
    and the damping resistor reverts to its original value. This
    narrows the loop bandwidth to its original cutoff frequency
    to allow better attenuation of the spurs than the wide-loop
    bandwidth.
    SPUR MECHANISMS
    The following section describes the three different spur mechan-
    isms that arise with a fractional-N synthesizer and how to
    minimize them in the ADF4153.
    Fractional Spurs
    The fractional interpolator in the ADF4153 is a third-order Σ-Δ
    modulator (SDM) with a modulus (MOD) that is programmable
    to any integer value from 2 to 4095. In low spur mode (dither
    enabled), the minimum allowed value of MOD is 50. The SDM
    is clocked at the PFD reference rate (FPFD) that allows PLL
    output frequencies to be synthesized at a channel step
    resolution of FPFD/MOD.
    In lowest noise mode and low noise and spur mode (dither off),
    the quantization noise from the Σ-Δ modulator appears as frac-
    tional spurs. The interval between spurs is FPFD/L, where L is the
    repeat length of the code sequence in the digital Σ-Δ modulator.
    For the third-order modulator used in the ADF4153, the repeat
    length depends on the value of MOD, as shown in Table 11.
    Table 11. Fractional Spurs with Dither Off
    Condition (Dither Off)
    Repeat
    Length
    Spur Interval
    If MOD is divisible by 2, but not 3
    2 × MOD
    Channel step/2
    If MOD is divisible by 3, but not 2
    3 × MOD
    Channel step/3
    If MOD is divisible by 6
    6 × MOD
    Channel step/6
    Otherwise
    MOD
    Channel step
    In low spur mode (dither enabled), the repeat length is
    extended to 221 cycles, regardless of the value of MOD, which
    makes the quantization error spectrum look like broadband
    noise. This can degrade the in-band phase noise at the PLL
    output by as much as 10 dB. Therefore, for lowest noise, dither
    off is a better choice, particularly when the final loop BW is low
    enough to attenuate even the lowest frequency fractional spur.
    Integer Boundary Spurs
    Another mechanism for fractional spur creation is interactions
    between the RF VCO frequency and the reference frequency.
    When these frequencies are not integer related (which is the
    point of a fractional-N synthesizer), spur sidebands appear on
    the VCO output spectrum at an offset frequency that corresponds
    to the beat note or difference frequency between an integer
    multiple of the reference and the VCO frequency.
    These spurs are attenuated by the loop filter and are more
    noticeable on channels close to integer multiples of the
    reference where the difference frequency can be inside the
    loop bandwidth, therefore, the name integer boundary spurs.
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