What stands between each technology and its target, classified by type, layer and severity. A gap held open by another technology points to it.
Projected cost stays in the hundreds of USD per tonne
criticalcostlayer: deploymentopen
Design and learning-curve estimates put the levelized cost of capture in the hundreds of USD per tonne: 94 to 232 USD/t for a designed aqueous-KOH plant (capture only, a design not an operating plant), and 341 to 374 USD/t of CO2 net removed with transport and storage at 1 Gt-CO2 per year of cumulative capacity. No source found for the cost of a plant operating today. Closing the gap needs cheaper sorbents, lower regeneration energy and cheaper storage.
Held open by: Low-cost CO2 sorbents, Geologic CO2 storage
Moving weights and cache costs more than the arithmetic
criticalengineeringlayer: systemactive
Each generated token streams the model weights and the key-value cache through memory, so memory traffic, not arithmetic, tends to bind the energy per token. The best published electrical die-to-die link measures 0.65 pJ/bit in a prototype, an interface-only figure. Closing the gap means fewer bytes moved (quantization, cache compression, sparse attention) and cheaper bytes.
Held open by: Low-energy data movement
Qubit count and control wiring
criticalengineeringlayer: systemactive
The largest error-corrected memory in the evidence uses 101 qubits; the target is up to a million. A coaxial line per qubit from room temperature does not scale, so control and readout must move into the cryostat. Cryo-CMOS multiplexing has worked below 15 mK without degrading relaxation times, and superconducting digital demultiplexing has run a multi-qubit system, both at laboratory scale.
Held open by: Cryogenic control electronics, Dilution refrigeration
Approaches
Gain of about 100 at power-plant repetition rates
criticalscientific unknownlayer: principleactive
The record target gain is 1.5, from a single shot at the National Ignition Facility. A plant needs a gain of about 100, which in turn needs a high fraction of the laser energy coupled to the target and the loss mechanisms from laser-plasma instabilities held down. Broadband lasers show promise against those instabilities, and simulations predict gains above 100 with less than 1 MJ of argon fluoride laser energy in direct drive, with no experiment yet at that gain.
Held open by: High-repetition-rate high-energy lasers
Approaches
Low sensitivity for stage I cancers
criticalscientific unknownlayer: principleactive
In the case-control validation study sensitivity rose with stage, from 16.8% at stage I to 90.1% at stage IV, so the test finds mostly cancers that are already advanced. Stage I is where early detection would matter most and where little tumour DNA reaches the blood.
Held open by: Low-cost DNA sequencing
Fixation shown in a landrace, not in high-yield cultivars
criticalscientific unknownlayer: systemactive
The high fixation share was measured in a landrace with aerial roots that secrete mucilage, grown in nitrogen-depleted soil. Moving the trait into elite cultivars at full yield, and under fertilization, has not been shown. Engineered root-associated bacteria that keep fixing in fertilized fields have been commercialized, but their abstract reports a yield gain over fertilizer alone, not a share of nitrogen from fixation.
Approaches
- Engineered root-associated diazotroph that fixes nitrogen despite fertilizer wen2021enabling
A working nitrogenase inside plant cells
criticalengineeringlayer: deviceactive
Expressing the nitrogenase components in plant mitochondria is the route to a crop that fixes its own nitrogen. Sixteen nitrogenase proteins have each been expressed and targeted to the mitochondrial matrix of a model plant, but the NifD component is the least abundant and a full working complex in a plant has not been shown.
Held open by: Plant genome engineering
Approaches
Success rate varies widely between targets and between groups
highscientific unknownlayer: deviceactive
The developers of one pipeline report experimental success rates of 10 to 100% depending on the target. An earlier study found the overall design success rate low and raised it nearly 10-fold with deep-learning filtering. An independent group testing another method on six targets, five designs each, reported that most targets gave no working binder.
Held open by: AI for science
Decoding is bound by memory bandwidth, not compute
highengineeringlayer: deviceactive
Small batches leave the arithmetic units idle while the memory system is saturated. The measured token energy falls from 7.46 to 0.72 J/token as output length grows from 10 to 512 tokens at batch 16, because fixed costs are amortized; batching gains shrink as context grows (6.31x at 512 tokens of context against 1.17x at 4K for 10 output tokens).
Held open by: Low-energy data movement
Idle capacity and small batches waste energy
highengineeringlayer: deploymentpromising
Production energy per prompt includes idle machine capacity and data-center overhead, not only active accelerator power. Google reports a 33x reduction in energy per median Gemini Apps text prompt over one year from software efficiency and clean-energy procurement (the abstract states the combined effect on energy and does not separate the two). Further gains depend on batching, routing and model choice.
Physical error rates uniform across the array
highengineeringlayer: deviceactive
Single pairs of superconducting qubits reach two-qubit gate fidelity of 99.94% (error 6e-4) with stability over 24 days, but a million-qubit machine needs every pair near that level at once, with leakage and crosstalk held down. The Willow memory ran at 0.143% logical error per cycle at distance 7, short of the target by about nine orders of magnitude. Closing it means both lower physical error and larger code distance on many more qubits.
Approaches
- Fluxonium qubits with direct two-qubit gates (TRL 3) lin2025days
Correlated errors from cosmic rays and radioactivity
highscientific unknownlayer: devicepromising
Muons and gamma rays create quasiparticle bursts that cause correlated errors across a chip, which error correction cannot absorb. A measurement on a 63-qubit processor separated the contributions of muons and gamma rays. Back-side phonon downconversion cut correlated poisoning by two orders of magnitude on three-qubit chips; it has not been shown on a million-qubit array.
Approaches
- Phonon downconversion with back-side normal-metal reservoirs (TRL 4) iaia2022phonon
Decoding at scale and in real time
highengineeringlayer: systemactive
The Willow decoder averaged 63 microseconds at distance 5, six times the 10 microsecond reaction time assumed in the RSA-2048 estimate, and at a cycle time of 1.1 microseconds, far from 1 microsecond at thousands of logical qubits. FPGA decoders report tens to hundreds of nanoseconds per measurement round in modeled-noise studies, which is not the same quantity as end-to-end latency in a running experiment.
Held open by: Real-time quantum error-correction decoder
Approaches
Refrigeration for the heat load
highengineeringlayer: systemopen
Each wired qubit adds passive heat load from cables and active load from signal dissipation. The strongest dilution refrigerator in the evidence delivers 2 mW at about 100 mK with a base temperature of 6.6 mK; no source in the atlas states the load of a million-qubit machine. Resource models of modular machines predict power and thermal load, and point to splitting the machine across cryostats.
Held open by: Dilution refrigeration
Approaches
Links between modules
highengineeringlayer: systemopen
A multinode machine needs entanglement between cryostats. Internode gates may be two to three orders of magnitude noisier and slower than local operations, and a systems analysis finds link performance must improve by 10 to 100 times.
Held open by: Quantum interconnect
Approaches
- Optical interconnects with entanglement distillation (TRL 2) ang2024arquin
Decoding rate is well below natural conversation
highengineeringlayer: systemactive
The 2023 demonstration decoded 62 words per minute, which the authors describe as beginning to approach the speed of natural conversation, 160 words per minute. The result comes from one participant, so how it generalizes across people is not established.
Held open by: Long-lived neural electrodes
Reuse of the whole launch system
highcostlayer: deploymentactive
Reusable first stages reduced launch cost, and providers on several continents plan reusable systems. The cost per kilogram falls with cumulative payload launched, following a learning curve, so further reductions depend on reuse at higher rate and with more of the vehicle recovered.
Practical plants already work near the thermodynamic limit
highfundamental limitlayer: principleopen
Reversible reverse osmosis and electrodialysis consume the Gibbs free energy of separation, and the practical energy of both approaches that minimum only as the number of stages grows. Reviews state that most desalination technologies already work near their limit, so the remaining reduction is bounded and each step costs capital. The numeric value of the minimum is in the body of the cited papers and is not recorded here yet.
Membrane permeability and selectivity trade off
highengineeringlayer: deviceactive
Reverse osmosis membranes trade water permeability against salt rejection. Analysis of biomimetic membranes indicates what a more permeable, defect-free membrane could offer for seawater desalination, but such membranes are not yet a commercial product.
Held open by: High-selectivity membranes
Benefit to patients not shown in a randomized trial
highscientific unknownlayer: deploymentopen
The NHS-Galleri randomized trial of 142,250 participants reported that its primary endpoint, a reduction in stage III/IV diagnoses in the test arm, was not met. Detecting cancers is not the same as improving outcomes; longer follow-up and other trials are needed.
Root-nodule symbiosis not yet engineered into non-legumes
highscientific unknownlayer: principleopen
Legumes host nitrogen-fixing rhizobia in root nodules. The objective of engineering nodulation in non-leguminous crops has not been achieved; the open questions are the signalling, infection and nodule-organogenesis programs.
Held open by: Plant genome engineering
CMOS logic has a ceiling of about two hundred times today's efficiency
mediumfundamental limitlayer: principleopen
Ho, Erdil and Besiroglu estimate a ceiling of 4.7e15 FP4 operations per joule for CMOS microprocessors, roughly two hundred times current microprocessors, from switching, interconnect capacitance and leakage. The atlas has no sourced current FLOP-per-joule value for deployed accelerators yet, so this gap has no metric of its own.
Held open by: Beyond-CMOS logic
Delivered power and cooling bound token output
mediumengineeringlayer: deploymentactive
At deployment scale the binding constraint can move from peak compute to delivered data-center power, cooling capacity and PUE. Embedded microfluidic cooling supports about 1e3 W/cm2; accelerator power density keeps rising.
Held open by: High-flux heat removal
Market structure and orbital debris may slow the decline
mediumregulationlayer: deploymentopen
The study that fits the learning curve warns that geopolitical shifts, possible monopolistic behavior in commercial launch markets and the growing problem of orbital debris may temper the cost reductions.
Reagent price is not the cost of a genome
mediumcostlayer: deploymentopen
The per-gigabase price quoted by a platform developer leaves out what NHGRI counts as production cost: labor, instruments amortized over three years, informatics and data submission. The atlas has no independent figure for the full cost of a 30-fold human genome today, so the current value is a derived, developer-reported number.
Low loss and active devices in one process
mediummanufacturinglayer: manufacturingactive
Silicon nitride gives the lowest waveguide loss, and integrating III-V and silicon materials has made large-scale nitride circuits with lasers and detectors possible. Ultra-low loss has been reached in an anneal-free process at no more than 250 C, which is compatible with CMOS back-end steps; keeping that loss while lasers, modulators and detectors share the chip, at volume, is the open problem.