Application Note: LoRa Modulation Crystal Oscillator Guidance

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WIRELESS & SENSING PRODUCTS Application Note: LoRa Modulation Crystal Oscillator Guidance AN1200.14 Rev 2.1 August 2018 www.semtech.com

Table of Contents 1. Introduction... 3 2. LoRa Modulation... 3 3. LoRa Modulation Crystal Specification... 3 3.1. Frequency Tolerance... 4 3.2. G Acceleration Sensitivity... 5 4. Recommended Crystal Manufacturers... 8 5. Recommended 32 MHz TCXO Manufacturers for Specific Applications if Required... 8 6. Conclusion... 9 7. Revision History... 9 8. References... 9 List of Figures Figure 1: LoRa PER versus Relative Crystal Oscillator Frequency Offset... 4 Figure 2: Instantaneous Frequency during one Vibration Cycle... 5 Figure 3: Effect of Acceleration due to Shock on a Crystal-Referenced PLL Transmitted Carrier... 6 Figure 4: Magnitude of Acceleration Relative to Crystal Package... 7 List of Tables Table 1: Typical Crystal Specification... 3 Table 2: LoRa Modulation Recommended Crystal Manufacturers... 8 Table 3: LoRa Modulation Recommended TCXO Manufacturers... 8 Page 2 of 10

1. Introduction The purpose of this application note is to assist the engineer with the selection of a suitable crystal oscillator for the LoRa modulation family of long-range wireless ISM transceiver devices. It is recommended to read this application note in conjunction with Application Note AN1200.07, Improving the Accuracy of a Crystal Oscillator [1], for further information on crystal oscillator specifications and parameters. 2. LoRa Modulation The LoRa modulation is a spread-spectrum technique that uses wideband linear frequency modulated pulses to encode information, whose frequency increases or decreases over a certain amount of time. As with other spread-spectrum modulation techniques, LoRa uses the entire channel bandwidth to broadcast a signal, making it robust to channel noise. In addition, because LoRa modulation uses a broad band of the spectrum, it is also resistant to long term relative frequency error, multi-path fading and Doppler effects. 3. LoRa Modulation Crystal Specification The crystal specification for LoRa modulation is given in Table 1. It can be observed that the crystal specification for s family of LoRa modulation transceivers is similar to those of existing FSK ISM transceivers. Since the internal oscillator drive circuitry of transceivers are similar, no special IP is required to condition the oscillator. Table 1: Typical Crystal Specification Symbol Description Conditions Min Typ Max Unit F XOSC Crystal Frequency 26 32 32 MHz R S Crystal Series Resistance For SX1272 1 and SX1276-30 40 Ω R S Crystal Series Resistance For SX1276 2 only - 30 100 Ω C 0 Crystal Shunt Capacitance - 2.8 7 pf C FOOT External Foot Capacitance On each pin XTA and XTB 8 15 22 pf C LOAD Crystal Load Capacitance 6-12 pf F TOL Initial Frequency Tolerance - ±10 ±30 ppm F TEMP Temp. Characteristics Application specific - - - ppm F AGING Aging Characteristics Application specific - - - ppm G S Acceleration Sensitivity Application specific 3-2 - ppb/g 1 Crystals with Rs (max) > 40 ohms are only to be used with SX1276 designs 2 Crystals with Rs (max) < 40 ohms can be used with SX1272 and SX1276 designs 3 Refer to Section 4 Page 3 of 10

There are two crystal specifications that warrant further analysis: - Frequency Tolerance - G or Acceleration Sensitivity 3.1. Frequency Tolerance The frequency or calibration tolerance, expressed in ppm, is typically an application-specific parameter. Usually modulation techniques offering sensitivity performances similar to LoRa such as narrow-band FHSS or high spreading factor DSSS typically require a crystal oscillator tolerance of only a few ppm to ensure both frequency and symbol rate accuracy. As previously highlighted, the LoRa modulation technique is impervious to the relative initial frequency error (and subsequently symbol rate tolerance) between the transmitter and the receiver. This immunity to both frequency and symbol tolerance is illustrated in Figure 1. 50 PER as a Function of Frequency Offset (125 khz BW) 40 30 PER (%) 20 SF7 SF12 10 0-40 -35-30 -25-20 -15-10 -5 0 5 10 15 20 25 30 35 40 Frequency Offset (khz) Figure 1: LoRa PER versus Relative Crystal Oscillator Frequency Offset The figure indicates that frequency tolerances of typically ±25% of the LoRa modulation bandwidth can be withstood and still maintain a 10% PER link. This compares favorably with current high-link budget systems. Page 4 of 10

3.2. G Acceleration Sensitivity G or acceleration sensitivity is a measurement of the sensitivity of a crystal oscillator to acceleration, and describes a short-term or instantaneous frequency error. A crystal oscillator subject to acceleration or mechanical shock has a slightly different series resonant frequency than the same oscillator experiencing no acceleration. It has been observed that the magnitude of the frequency shift is proportional to both the magnitude and the direction of the acceleration relative to a coordinate system applied to the crystal. [2] A representation of this effect can be considered in the case of a crystal subject to a cycle of acceleration at a rate of f V : Figure 2: Instantaneous Frequency during one Vibration Cycle Page 5 of 10

Each plot shows the instantaneous output frequency sampled at a time period n/4*f V. If we consider the rate of acceleration to be sinusoidal, it can be observed that the instantaneous frequency deviation occurs at the crest and trough of the applied sinusoidal force. It can be shown that the magnitude of the instantaneous frequency deviation is proportional to the instantaneous amplitude of the acceleration. [2] This can be viewed practically by observing the effect of acceleration or shock on the spectrum of a phaselocked loop carrier implemented with a crystal oscillator that does not have a low-g sensitivity crystal specified, as illustrated in Figure 3. Applying an acceleration force to the crystal causes an instantaneous change in frequency. The apparent amplitude of the instantaneous frequency is limited only by the measurement instrumentation. Constant frequency (zero acceleration) Instantaneous change of frequency due to acceleration Figure 3: Effect of Acceleration due to Shock on a Crystal-Referenced PLL Transmitted Carrier Page 6 of 10

As it has been noted, the magnitude of the instantaneous frequency shift is also proportional to the direction of the acceleration relative to a coordinate system applied to the crystal. As illustrated in Figure 4 it can be observed that the resultant acceleration vector is proportional to both the magnitude of the acceleration, Γ G, and relative angle (Θ, Φ) applied. [3] SMD Crystal Package Figure 4: Magnitude of Acceleration Relative to Crystal Package Page 7 of 10

4. Recommended Crystal Manufacturers Crystal manufacturers familiar with the requirements for GPS receiver designs are able to recommend a suitable crystal for a given application and can also advise as to orientation. Loading capacitance must be applied externally and adapted to the actual Cload specifications of the crystal, to center the LO frequency. Load capacitors value can slightly vary depending on the selected crystal part number and PCB design. Currently LoRa transceiver reference designs use only 32 MHz low-g sensitivity crystals from the following manufacturers below. Contact directly a crystal manufacturer sales representative for more details and specifications by selecting the desired part number below: Table 2: LoRa Modulation Recommended Crystal Manufacturers Manufacturer Website Package Size Model / Reference Part Number Rakon http://temexpress.com/en/index 3.2x2.5mm FTR5092-A3 2 2.0x1.6mm FTR5123-B0 2 NDK http://www.ndk.com/en/products/search/crystal/index.html 2.5x2.0mm NX2520SA / EXS00A-CS00131 1 2.0x1.6mm NX2016SA / EX500A-CS06465 1 Epson http://www5.epsondevice.com/en/ic_partners/info.html 2.0x1.6mm 1 FA-128 / Q22FA1280053000 FA-128 / Q22FA1280058900 2 Taitien http://www.taitien.com/crystal-oscillator 3.2x2.5mm S0197-X-002-3 2 KDS http://www.kds.info/product/ 2.0x1.6mm DSX211SH-32MHz 1ZZHAE32000AA0B 2 3.2x2.5mm DSX321G-32MHz 1C232000AA0Q 2 Murata http://www.murata.com/en-global/products/quartzdevice/ 2.0x1.6mm XRCGB32M000F1H17R0 2 2 XRCGB32M000F1H18R0 Kyocera http://www.kyocera-crystal.jp/eng/prdct/list/xtal/#02 2.0x1.6mm CX2016DB32000F0FFFC2 1 NSK http://www.nsk.com.tw/product.asp?lv=0&id=2 2.0x1.6mm NXN32.000AG10F-DKAB12 2 1 Crystals with Rs (max) > 40 ohms are only to be used with SX1276 designs 2 Crystals with Rs (max) < 40 ohms can be used with SX1272 and SX1276 designs 5. Recommended 32 MHz TCXO Manufacturers for Specific Applications if Required Table 3: LoRa Modulation Recommended TCXO Manufacturers Manufacturer Website Package Size Model / Reference Part Number NDK http://www.ndk.com/en/products/search/tcxo/index.html 2.0x1.6mm NT2016SA / END4263A 2.0x1.6mm NT2016SB / END4329A Rakon http://temexpress.com/en/index 3.2x2.5mm IT3205CE 32.000MHz 2.0x1.6mm IT2105 32.000MHz Taitien http://www.taitien.com/vctcxo-tcxo 3.2x2.5mm S0197-T-004-3 KDS http://www.kds.info/product/ 2.0x1.6mm T16-0626A-DSB211SDN-32MHz- 1XXD32000PCA Kyocera http://www.kyocera-crystal.jp/eng/prdct/list/tcxo/ 2.0x1.6mm KT2016K32000ACW18YAS Page 8 of 10

6. Conclusion Since LoRa modulation contains both relative time and frequency information it can be deduced that any short-term frequency variance could lead to incorrect detection of encoded data. Thus it is recommended that for those applications which may be subject to acceleration forces, such as shock or vibration, for example where the SX1272 transceiver is implemented in a mobile link (such as a hand-held or vehicle mounted application) a low-g crystal is used as the reference oscillator. In addition, since the resultant acceleration vector has both magnitude and angle components, care should be taken to ensure that both crystal and PCB orientation minimize the acceleration vector. If in doubt, contact your crystal vendor or representative. 7. Revision History Version Date Modifications 1 August 2013 First Release 2 July 2017 Update of crystal manufacturers for 32.0 MHz Crystal and TCXO Migration to the new document template 2.1 August 2018 Update of Murata crystal models Correction of references Addition of a Revision History chapter 8. References [1] Application Note AN1200.07, Improving the Accuracy of a Crystal Oscillator https://www.semtech.com/uploads/documents/xo_precision_std.pdf [2] The Acceleration Sensitivity of Quartz Crystal Oscillators: A Review, Raymond L Filler (IEEE Transactions on Ultrasonics, Ferroelectrics and Frequency Control, Vol. 35, No.3 May 1988) [3] Greenway Industries Application Note, Acceleration Sensitivity of Characteristics of Quartz Crystal Oscillators Page 9 of 10

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