High speed telemetry system using transmission medium as a...

Surgery: light – thermal – and electrical application – Light – thermal – and electrical application – Electrical therapeutic systems

Reexamination Certificate

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Reexamination Certificate

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06301504

ABSTRACT:

FIELD OF THE INVENTION
The present invention relates generally to cardiac pacemakers, and other types of implantable medical devices that can be programmed and/or analyzed following implantation using an external diagnostic/programmer system. Particularly, the invention relates to a high speed digital telemetry system for use in implantable devices. More specifically, the present invention relates to an implantable high bit rate telemetry transmitter and corresponding external receiver that utilize the transmission medium as a component of the telemetry link
BACKGROUND OF THE INVENTION
Implantable devices are implanted in a human or animal for the purpose of performing a desired function. This function may be purely observational or experimental in nature, such as monitoring certain body functions; or it may be therapeutic or regulatory in nature, such as providing critical electrical stimulation pulses to certain body tissue, nerves or organs for the purpose of causing a desired response. Implantable medical devices such as pacemakers, perform both observational and regulatory functions, i.e., they monitor the heart to ensure it beats at appropriate intervals; and if not, they cause an electrical stimulation pulse to be delivered to the heart in an attempt to force the heart to beat at an appropriate rate.
In order for an implantable device to perform its functions at minimum inconvenience and risk to the person or animal within whom it is used, some sort of noninvasive telemetry means must be provided that allows data and commands to be easily passed back and forth between the implantable device and an external device. Such an external device, known by a variety of names, such as a controller, programmer, or monitor, provides a convenient mechanism through which the operation of the implantable device can be controlled and monitored, and through which data sensed or detected by the implantable device can be transferred out of the implantable device to an external (non-implanted) location where it can be read, interpreted, or otherwise used in a constructive manner.
As the sophistication and complexity of implantable devices has increased in recent years, the amount of data that must be transferred between an implantable device and its accompanying external device or programmer, has dramatically increased. This, in turn, has resulted in a search for more efficient ways to effectuate such a data transfer at high speed. The telemetry must not only transfer the desired data without significant error, but it must do so at a high speed while preserving the limited power resources of the implanted device.
Currently, three basic techniques have been used for communicating with an implantable device: (1) static magnetic field coupling; (2) reflected impedance coupling; and (3) RF coupling. In static magnetic field coupling, a static magnetic field is generated externally to the implanted device by using a permanent magnet, having sufficient strength to close (or open) a magnetic reed switch within the implanted device. While such a technique provides a fairly reliable mechanism for turning various functions within the implanted device ON or OFF, such as turning the telemetry circuits within an implanted device ON only when an external telemetry head is positioned a few inches from the implanted device, the technique is much too slow for efficiently transferring any significant amount of data. Further, for all practical purposes, the static magnetic system is mainly useful for transferring commands or data to the implanted device, not for transferring data or commands from the implanted device. This is because the weight and/or power requirements associated with the types of permanent magnets or electromagnets needed to operate a magnetic reed switch several inches distant therefrom is incompatible with the requirements of most implantable devices.
In a reflected impedance coupling system, information is transferred using the reflected impedance of an internal (implanted) L-R or L-C circuit energized by an inductively coupled, external L-R or L-C circuit. Such a system is shown, for example, in U.S. Pat. No. 4,223,679. While such a system uses little or no current to transmit information, the speed at which the information is transferred is quite limited. The external circuit uses an RF (radio frequency) magnetic field carrier. In the cited patent, a voltage controlled oscillator (VCO), in the implanted device, is controlled by the signal to be telemetered. The VCO, in turn, varies the impedance that is reflected. If the signal controlling the VCO is a binary digital signal (having two possible values, e.g., a binary “1” and a binary “0”), this signal encodes the VCO so that the VCO varies from one frequency (representing a binary “1”) to another frequency (representing a binary “0”). This technique is known as frequency shift keying (FSK). Each bit duration, i.e., the time in which the binary digit (bit) is expressed, requires a number of carrier cycles. Hence, the bit rate cannot generally be much higher than 10% to 30% of the VCO center frequency. On the other hand, the RF carrier frequency cannot be too high because of the metal enclosure of the implanted device acts as a low pass, single pole filter having an upper cut-off frequency of between 10-30 kHz. Further, the external oscillator L-C circuit typically has a Q (quality factor) of 20 to 50, meaning that the useful modulation bandwidth is limited to around 2 to 5 percent of the RF carrier frequency. This means that a 36 kHz carrier is typically only able to transmit data at a data rate of from 72 to 540 bits per second (bps). Such a rate is generally considered inadequate for modern implantable devices, which devices may have thousands of bits of data to be transmitted.
In an RF coupled system, information is transferred from a transmitting coil to a receiving coil by way of a carrier signal. The carrier signal is modulated with the data that is to be transmitted using an appropriate modulation scheme, such as FSK or PSK (phase-shift keying for reversing the phase of the carrier by 180 degrees). The modulated carrier induces a voltage at the receiving coil that tracks the modulated carrier signal. This received signal is then demodulated in order to recover the transmitted data. Because of the metal enclosure of the implanted device, which acts as a low pass filter (attenuating high frequencies), the carrier frequency cannot be increased above approximately 10-20 kHz without an unacceptable increase in transmitting coil power. Further, depending upon the type of modulation/demodulation scheme employed, the data or bit rate cannot exceed a prescribed fraction of the carrier frequency, without exceeding a specified amount of mutual interference, i.e., without being able to reliably distinguish between a modulation that represents a binary “1” and modulation that represents a binary “0”.
The maximum data transfer rate (bit rate) at which independent signal values can be transmitted over a specified channel without exceeding a specified amount of mutual interference is referred to as the “Nyquist rate.” The maximum allowable Nyquist rate is directly related to the bandwidth of the channel through which the data is transferred. Conversely, the “Nyquist bandwidth” is that bandwidth required to allow independent signal values to be transmitted at a given rate without exceeding the specified levels of mutual interference. For example, if the bandwidth of the channel through which the data is transferred is W, the Nyquist rate (assuming an ideal channel) may be as high as 2W. Stated differently, if the data rate is 2W, the Nyquist bandwidth must be at least W. Because of these and other limitations, conventional implantable devices using RF coupling have generally not been able to transfer data at rates in excess of 2-4 kbps. It should be noted that a one-sided bandwidth definition is used, namely that a bandwidth W refers to a range of frequencies from 0 to W, or from −W to 0. Where a carrier signal having a frequency f
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