# Module ristretto_bulletproofs::notes[−][src]

This module contains notes on how and why Bulletproofs work.

The documentation is laid out roughly as follows. General notes on the range proof and inner-product proofs are here. The description of each protocol is contained in the respective range_proof and inner_product_proof modules. Finally, structs from those modules are publicly re-exported from the crate root, so that the external documentation describes how to use the API, while the internal documentation describes how it works.

# Notation

We change notation from the original Bulletproofs paper. The primary motivation is that our implementation uses additive notation, and we would like our description of the protocol to use the same notation as the implementation.

In general, we use lower-case letters $$a, b, c$$ for scalars in $${\mathbb Z_p}$$ and upper-case letters $$G,H,P,Q$$ for group elements in $${\mathbb G}$$. Vectors are denoted as $${\mathbf{a}}$$ and $${\mathbf{G}}$$, and the inner product of two vectors is denoted by $${\langle -, - \rangle}$$. Notice that $${\langle {\mathbf{a}}, {\mathbf{b}} \rangle} \in {\mathbb Z_p}$$ produces a scalar, while $${\langle {\mathbf{a}}, {\mathbf{G}} \rangle} \in {\mathbb G}$$ is a multiscalar multiplication. The vectors of all $$0$$ and all $$1$$ are denoted by $${\mathbf{0}}$$, $${\mathbf{1}}$$ respectively.

Vectors are indexed starting from $$0$$, unlike the paper, which indexes from $$1$$. For a scalar $$y$$, we write \begin{aligned} {\mathbf{y}}^{n} &= (1,y,y^{2},\ldots,y^{n-1}) \end{aligned} for the vector whose $$i$$-th entry is $$y^{i}$$. For vectors $${\mathbf{v}}$$ of even length $$2k$$, we define $${\mathbf{v}}_{\operatorname{lo}}$$ and $${\mathbf{v}}_{\operatorname{hi}}$$ to be the low and high halves of $${\mathbf{v}}$$: \begin{aligned} {\mathbf{v}}_{\operatorname{lo}} &= (v_0, \ldots, v_{k-1})\\ {\mathbf{v}}_{\operatorname{hi}} &= (v_{k}, \ldots, v_{2k-1}) \end{aligned} Pedersen commitments are written as \begin{aligned} \operatorname{Com}(v) &= \operatorname{Com}(v, {\widetilde{v}}) = v \cdot B + {\widetilde{v}} \cdot {\widetilde{B}}, \end{aligned} where $$B$$ and $${\widetilde{B}}$$ are the generators used for the values and blinding factors, respectively. We denote the blinding factor for the value $$v$$ by $${\widetilde{v}}$$, so that it is clear which blinding factor corresponds to which value, and write $$\operatorname{Com}(v)$$ instead of $$\operatorname{Com}(v, {\widetilde{v}})$$ for brevity.

We also make use of vector Pedersen commitments, which we define for pairs of vectors as \begin{aligned} \operatorname{Com}({\mathbf{a}}_{L}, {\mathbf{a}}_{R}) &= \operatorname{Com}({\mathbf{a}}_{L}, {\mathbf{a}}_{R}, {\widetilde{a}}) = {\langle {\mathbf{a}}_{L}, {\mathbf{G}} \rangle} + {\langle {\mathbf{a}}_{R}, {\mathbf{H}} \rangle} + {\widetilde{a}} {\widetilde{B}},\end{aligned} where $${\mathbf{G}}$$ and $${\mathbf{H}}$$ are vectors of generators. Notice that this is exactly the same as taking a commitment to the vector of values $${\mathbf{a}}_{L} \Vert {\mathbf{a}}_{R}$$ with the vector of bases $${\mathbf{G}} \Vert {\mathbf{H}}$$, but defining the commitment on pairs of vectors is a more convenient notation.

The variable renaming is as follows: \begin{aligned} g &\xrightarrow{} B & \gamma &\xrightarrow{} \tilde{v} \\ h &\xrightarrow{} \tilde{B} & \alpha &\xrightarrow{} \tilde{a} \\ {\mathbf{g}} &\xrightarrow{} {\mathbf{G}} & \rho &\xrightarrow{} \tilde{s} \\ {\mathbf{h}} &\xrightarrow{} {\mathbf{H}} & \tau_i &\xrightarrow{} \tilde{t}_i \\ & & \mu &\xrightarrow{} \tilde{e} \\ \end{aligned}

# Range Proofs from inner products

The goal of a range proof is for a prover to convince a verifier that a particular value $$v$$ lies within a valid range, without revealing any additional information about the value $$v$$.

The prover begins with a secret value $$v$$ and commitment $$V = \operatorname{Com}(v)$$, which it sends to the verifier. The prover wishes to convince the verifier that \begin{aligned} v &\in [0, 2^{n}) \end{aligned} without revealing $$v$$.

Since the prover will eventually use an inner product proof to do this, we want to work towards expressing this condition in terms of a single inner product. In this section, we construct successive statements which imply $$v \in [0,2^{n})$$ until we arrive at the ones the prover will use to convince the verifier.

## Proving range statements with bit vectors

Let $${\mathbf{a}}$$ be the vector of bits of $$v$$. Then $$v$$ can be represented as an inner product of bits $${\mathbf{a}}$$ and powers of two $${\mathbf{2}}^{n} = (1,2,4,\ldots,2^{n-1})$$: \begin{aligned} v &= {\langle {\mathbf{a}}, {\mathbf{2}}^{n} \rangle} \\ &= a_{0}\cdot 2^0 + \dots + a_{n-1}\cdot 2^{n-1}. \end{aligned} We need $${\mathbf{a}}$$ to be a vector of integers $$\{0,1\}$$. This can be expressed with an additional condition ${\mathbf{a}} \circ ({\mathbf{a}} - {\mathbf{1}}) = {\mathbf{0}},$ where $${\mathbf{x}} \circ {\mathbf{y}}$$ denotes the entry-wise multiplication of two vectors. The result of multiplication can be all-zero if and only if every bit is actually $$0$$ or1 $$1$$.

As a result of representing value in binary, the range condition $$v \in [0, 2^{n})$$ is equivalent to the pair of conditions \begin{aligned} {\langle {\mathbf{a}}, {\mathbf{2}}^{n} \rangle} &= v, \\ {\mathbf{a}} \circ ({\mathbf{a}} - {\mathbf{1}}) &= {\mathbf{0}}. \end{aligned} We will eventually need to make separate commitments to the vectors $${\mathbf{a}}$$ and $${\mathbf{a}} - {\mathbf{1}}$$, so we set $${\mathbf{a}}_{L} = {\mathbf{a}}$$, $${\mathbf{a}}_{R} = {\mathbf{a}} - {\mathbf{1}}$$ to obtain \begin{aligned} {\langle {\mathbf{a}}_{L}, {\mathbf{2}}^{n} \rangle} &= v, \\ {\mathbf{a}}_{L} \circ {\mathbf{a}}_{R} &= {\mathbf{0}}, \\ ({\mathbf{a}}_{L} - {\mathbf{1}}) - {\mathbf{a}}_{R} &= {\mathbf{0}}. \end{aligned}

## Proving vectors of statements with a single statement

The statements above are statements about vectors, or equivalently, a vector of statements about each entry. We want to combine all of these into a single statement.

First, we will combine each of the two vector-statements into a single statement. Since $${\mathbf{b}} = {\mathbf{0}}$$ if and only if2 $${\langle {\mathbf{b}}, {\mathbf{y}}^{n} \rangle} = 0$$ for every $$y$$, the statements above are implied by \begin{aligned} {\langle {\mathbf{a}}_{L}, {\mathbf{2}}^{n} \rangle} &= v, \\ {\langle {\mathbf{a}}_{L} - {\mathbf{1}} - {\mathbf{a}}_{R}, {\mathbf{y}}^{n} \rangle} &= 0, \\ {\langle {\mathbf{a}}_{L}, {\mathbf{a}}_{R} \circ {\mathbf{y}}^{n} \rangle} &= 0 \end{aligned} for the verifier’s choice of a challenge value $$y$$.

The three resulting statements can then be combined in the same way, using the verifier’s choice of $$z$$: \begin{aligned} z^{2} v &= z^{2} {\langle {\mathbf{a}}_{L}, {\mathbf{2}}^{n} \rangle} + z {\langle {\mathbf{a}}_{L} - {\mathbf{1}} - {\mathbf{a}}_{R}, {\mathbf{y}}^{n} \rangle} + {\langle {\mathbf{a}}_{L}, {\mathbf{a}}_{R} \circ {\mathbf{y}}^{n} \rangle} \end{aligned}

## Combining inner products

Finally, we want to combine these terms into a single inner product. Our goal is to rearrange the inner product above so that terms involving $${\mathbf{a}}_{L}$$ appear only on the left-hand side, terms involving $${\mathbf{a}}_{R}$$ appear only on the right-hand side, and non-secret terms (which the verifier can compute on its own) are factored out into a new term $$\delta$$.

First, break the statement into simpler terms, then rearrange: \begin{aligned} z^2 v &= z^2 {\langle {\mathbf{a}}_{L}, {\mathbf{2}}^n \rangle} + z {\langle {\mathbf{a}}_{L}, {\mathbf{y}}^n \rangle} - z {\langle {\mathbf{a}}_{R}, {\mathbf{y}}^n \rangle} - z {\langle {\mathbf{1}}, {\mathbf{y}}^n \rangle} + {\langle {\mathbf{a}}_{L}, {\mathbf{a}}_{R} \circ {\mathbf{y}}^n \rangle} \\ z^{2} v + z {\langle {\mathbf{1}}, {\mathbf{y}}^{n} \rangle} &= z^2 {\langle {\mathbf{a}}_{L}, {\mathbf{2}}^n \rangle} + z {\langle {\mathbf{a}}_{L}, {\mathbf{y}}^n \rangle} - z {\langle {\mathbf{1}} , {\mathbf{a}}_{R} \circ {\mathbf{y}}^n \rangle} + {\langle {\mathbf{a}}_{L}, {\mathbf{a}}_{R} \circ {\mathbf{y}}^n \rangle} \\ z^{2} v + z {\langle {\mathbf{1}}, {\mathbf{y}}^{n} \rangle} &= {\langle {\mathbf{a}}_{L}, z^{2} {\mathbf{2}}^n \rangle} + {\langle {\mathbf{a}}_{L}, z {\mathbf{y}}^n \rangle} + {\langle -z {\mathbf{1}} , {\mathbf{a}}_{R} \circ {\mathbf{y}}^n \rangle} + {\langle {\mathbf{a}}_{L}, {\mathbf{a}}_{R} \circ {\mathbf{y}}^n \rangle} \\ z^{2} v + z {\langle {\mathbf{1}}, {\mathbf{y}}^{n} \rangle} &= {\langle {\mathbf{a}}_{L}, z^{2} {\mathbf{2}}^n + z {\mathbf{y}}^{n} + {\mathbf{a}}_{R} \circ {\mathbf{y}}^{n} \rangle} + {\langle -z {\mathbf{1}} , {\mathbf{a}}_{R} \circ {\mathbf{y}}^n \rangle} \end{aligned} To combine the terms on the right-hand side, add $${\langle -z {\mathbf{1}}, z^2 {\mathbf{2}}^n + z {\mathbf{y}}^n \rangle}$$ to each side, then simplify: \begin{aligned} z^{2} v + z {\langle {\mathbf{1}}, {\mathbf{y}}^{n} \rangle} - {\langle z {\mathbf{1}}, z^2 {\mathbf{2}}^n + z {\mathbf{y}}^n \rangle} &= {\langle {\mathbf{a}}_{L}, z^{2} {\mathbf{2}}^n + z {\mathbf{y}}^{n} + {\mathbf{a}}_{R} \circ {\mathbf{y}}^{n} \rangle} \\ &+ {\langle -z {\mathbf{1}} , z^2 {\mathbf{2}}^n + z {\mathbf{y}}^n + {\mathbf{a}}_{R} \circ {\mathbf{y}}^n \rangle} \\ z^2 v + (z - z^2) {\langle {\mathbf{1}}, {\mathbf{y}}^n \rangle} - z^3 {\langle {\mathbf{1}}, {\mathbf{2}}^n \rangle} &= {\langle {\mathbf{a}}_{L} - z{\mathbf{1}}, z^{2} {\mathbf{2}}^n + z {\mathbf{y}}^{n} + {\mathbf{a}}_{R} \circ {\mathbf{y}}^{n} \rangle} \end{aligned} Combining all non-secret terms outside the inner product $\delta(y,z) = (z - z^{2}) {\langle {\mathbf{1}}, {\mathbf{y}}^{n} \rangle} - z^{3} {\langle {\mathbf{1}}, {\mathbf{2}}^{n} \rangle},$ we finally obtain $z^{2}v + \delta(y,z) = {\langle {\mathbf{a}}_{L} - z {\mathbf{1}}, {\mathbf{y}}^{n} \circ ({\mathbf{a}}_{R} + z {\mathbf{1}}) + z^{2} {\mathbf{2}}^{n} \rangle}.$ This is equivalent to the original inner-product equation, but has a single inner product with $${\mathbf{a}}_{L}$$ on the left, $${\mathbf{a}}_{R}$$ on the right, and non-secret terms factored out.

## Blinding the inner product

The prover cannot send the left and right vectors in the single inner-product equation to the verifier without revealing information about the value $$v$$, and since the inner-product argument is not zero-knowledge, they cannot be used there either.

Instead, the prover chooses vectors of blinding factors ${\mathbf{s}}_{L}, {\mathbf{s}}_{R} \;{\xleftarrow{\}}\; {\mathbb Z_p}^{n},$ and uses them to construct vector polynomials \begin{aligned} {\mathbf{l}}(x) &= {\mathbf{l}}_{0} + {\mathbf{l}}_{1} x = ({\mathbf{a}}_{L} + {\mathbf{s}}_{L} x) - z {\mathbf{1}} & \in {\mathbb Z_p}[x]^{n} \\ {\mathbf{r}}(x) &= {\mathbf{r}}_{0} + {\mathbf{r}}_{1} x = {\mathbf{y}}^{n} \circ \left( ({\mathbf{a}}_{R} + {\mathbf{s}}_{R} x\right) + z {\mathbf{1}}) + z^{2} {\mathbf{2}}^{n} &\in {\mathbb Z_p}[x]^{n} \end{aligned} These are the left and right sides of the combined inner product with $${\mathbf{a}}_{L}$$, $${\mathbf{a}}_{R}$$ replaced by blinded terms $${\mathbf{a}}_{L} + {\mathbf{s}}_{L} x$$, $${\mathbf{a}}_{R} + {\mathbf{s}}_{R} x$$. Notice that since only the blinding factors $${\mathbf{s}}_{L}$$, $${\mathbf{s}}_{R}$$ are multiplied by $$x$$, the vectors $${\mathbf{l}}_{0}$$ and $${\mathbf{r}}_{0}$$ are exactly the left and right sides of the unblinded single inner-product: ${\langle {\mathbf{l}}_{0}, {\mathbf{r}}_{0} \rangle} = z^{2}v + \delta(y,z)$

Setting $t(x) = {\langle {\mathbf{l}}(x), {\mathbf{r}}(x) \rangle} = t_{0} + t_{1} x + t_{2} x^{2},$ we can express the coefficients of $$t(x)$$ using Karatsuba’s method: \begin{aligned} t_{0} &= {\langle {\mathbf{l}}_{0}, {\mathbf{r}}_{0} \rangle}, \\ t_{2} &= {\langle {\mathbf{l}}_{1}, {\mathbf{r}}_{1} \rangle}, \\ t_{1} &= {\langle {\mathbf{l}}_{0} + {\mathbf{l}}_{1}, {\mathbf{r}}_{0} + {\mathbf{r}}_{1} \rangle} - t_{0} - t_{2} \end{aligned} Since \begin{aligned} t_{0} &= {\langle {\mathbf{a}}_{L} - z {\mathbf{1}}, {\mathbf{y}}^{n} \circ ({\mathbf{a}}_{R} + z {\mathbf{1}}) + z^{2} 2^{n} \rangle},\end{aligned} for the prover to convince the verifier that the unblinded single inner-product equation holds, it’s enough to prove that the constant term $$t_{0}$$ of $$t(x)$$ is $$z^{2} v + \delta(y,z)$$, and that this $$t(x)$$ is the correct polynomial. Proving that $$t(x)$$ is correct means proving that $${\mathbf{l}}(x)$$, $${\mathbf{r}}(x)$$ are correctly formed, and that $$t(x) = {\langle {\mathbf{l}}(x), {\mathbf{r}}(x) \rangle}$$.

## Proving that $$t_{0}$$ is correct

In order to prove that the constant term of $$t(x)$$ is $$z^{2} v + \delta(y,z)$$, the prover first forms a commitment to the coefficients of $$t(x)$$, then convinces the verifier that these commit to the correct $$t(x)$$ by evaluating the polynomial at a challenge point $$x$$.

The prover has already used $$V = \operatorname{Com}(v)$$ to commit to $$v$$ (and hence to $$t_{0}$$), so the prover forms commitments $$T_{1} = \operatorname{Com}(t_{1})$$ and $$T_{2} = \operatorname{Com}(t_{2})$$, then sends these to the verifier. The commitments $$V$$, $$T_{1}$$, $$T_{2}$$ are related to each other and to $$t(x)$$ by the following diagram: \begin{aligned} t(x) B &\quad &= \quad & z^{2}vB & \quad &+ \quad & \delta(y,z) B & \quad &+ \quad& x t_{1} B &\quad &+\quad & x^2 t_{2} B \\ + &\quad & \quad & + & \quad & \quad & + & \quad & \quad& + &\quad & \quad & + \\ {\tilde{t}}(x) {\widetilde{B}} &\quad &= \quad & z^2 {\widetilde{v}} {\widetilde{B}} & \quad &+ \quad & 0 {\widetilde{B}} & \quad &+ \quad& x {\tilde{t}}_{1} {\widetilde{B}} &\quad &+\quad & x^{2} {\tilde{t}}_{2} {\widetilde{B}} \\ \shortparallel &\quad & \quad & \shortparallel & \quad & \quad & \shortparallel & \quad & \quad& \shortparallel &\quad & \quad & \shortparallel \\ &\quad &= \quad & z^2 V & \quad &+ \quad & \delta(y,z) B & \quad &+ \quad& x T_{1} &\quad &+\quad & x^{2} T_{2} \end{aligned} Notice that the sum of each column is a commitment to the variable in the top row using the blinding factor in the second row. The sum of all of the columns is $$t(x) B + {\tilde{t}}(x) {\widetilde{B}}$$, a commitment to the value of $$t$$ at the point $$x$$, using the synthetic blinding factor3 ${\tilde{t}}(x) = z^{2} {\tilde{v}} + x {\tilde{t}}_{1} + x^{2} {\tilde{t}}_{2}.$ To convince the verifier that $$t(x) = z^2v + \delta(y,z) + t_{1} x + t_{2} x^{2}$$, the prover sends the opening $$t(x), {\tilde{t}}(x)$$ to the verifier, who uses the bottom row of the diagram to check consistency: $t(x) B + {\tilde{t}}(x) {\widetilde{B}} \stackrel{?}{=} z^2 V + \delta(y,z) B + x T_{1} + x^{2} T_{2}.$

## Proving that $${\mathbf{l}}(x)$$, $${\mathbf{r}}(x)$$ are correct

We want to relate $${\mathbf{l}}(x)$$ and $${\mathbf{r}}(x)$$ to commitments to $${\mathbf{a}}_{L}$$, $${\mathbf{a}}_{R}$$, $${\mathbf{s}}_{L}$$, and $${\mathbf{s}}_{R}$$. However, since \begin{aligned} {\mathbf{r}}(x) &= {\mathbf{y}}^{n} \circ \left( ({\mathbf{a}}_{R} + {\mathbf{s}}_{R} x\right) + z {\mathbf{1}}) + z^{2} {\mathbf{2}}^{n},\end{aligned} we need commitments to $${\mathbf{y}}^{n} \circ {\mathbf{a}}_{R}$$ and $${\mathbf{y}}^{n} \circ {\mathbf{s}}_{R}$$. However, since the prover must form commitments before receiving the verifier’s challenge $$y$$, the prover can only commit to $$a_{R}$$ and $$s_{R}$$. Since the prover’s commitments are to $$a_{R}$$ and $$s_{R}$$, the verifier needs to transmute the prover’s commitment $$\operatorname{Com}({\mathbf{a}}_{L},{\mathbf{a}}_{R}, {\widetilde{a}})$$ into a commitment $$\operatorname{Com}({\mathbf{a}}_{L}, {\mathbf{y}}^{n} \circ {\mathbf{a}}_{R}, {\widetilde{a}})$$ (and similarly for $${\mathbf{s}}_{R}$$). To do this, notice that \begin{aligned} \operatorname{Com}({\mathbf{a}}_{L}, {\mathbf{a}}_{R}, {\widetilde{a}}) &= {\langle {\mathbf{a}}_{L}, {\mathbf{G}} \rangle} + {\langle {\mathbf{a}}_{R}, {\mathbf{H}} \rangle} + {\widetilde{a}} {\widetilde{B}} \\ &= {\langle {\mathbf{a}}_{L}, {\mathbf{G}} \rangle} + {\langle {\mathbf{y}}^{n} \circ {\mathbf{a}}_{R}, {\mathbf{y}}^{-n} \circ {\mathbf{H}} \rangle} + {\widetilde{a}} {\widetilde{B}}, \end{aligned} so that by changing generators to $${\mathbf{H}}' = {\mathbf{y}}^{-n} \circ {\mathbf{H}}$$, the point which is a commitment to $$({\mathbf{a}}_{L}, {\mathbf{a}}_{R}, {\widetilde{a}})$$ with respect to $$({\mathbf{G}}, {\mathbf{H}}, {\widetilde{a}})$$ is transmuted into a commitment to $$({\mathbf{a}}_{L}, {\mathbf{y}}^{n} \circ {\mathbf{a}}_{R}, {\widetilde{a}})$$ with respect to $$({\mathbf{G}}, {\mathbf{H}}', {\widetilde{a}})$$.

To relate the prover’s commitments $$A = \operatorname{Com}({\mathbf{a}}_{L}, {\mathbf{a}}_{R})$$ and $$S = \operatorname{Com}({\mathbf{s}}_{L}, {\mathbf{s}}_{R})$$ to $${\mathbf{l}}(x)$$ and $${\mathbf{r}}(x)$$, we use the following diagram: \begin{aligned} {\langle {\mathbf{l}}(x), {\mathbf{G}} \rangle} &\quad &= \quad & {\langle {\mathbf{a}}_L, {\mathbf{G}} \rangle} & \quad &+ \quad & x {\langle {\mathbf{s}}_L, {\mathbf{G}} \rangle} &\quad &+\quad & {\langle -z{\mathbf{1}}, {\mathbf{G}} \rangle} \\ + &\quad & \quad & + & \quad & \quad & + &\quad & \quad & + \\ {\langle {\mathbf{r}}(x), {\mathbf{H}}' \rangle} &\quad &= \quad & {\langle {\mathbf{a}}_R, {\mathbf{H}} \rangle} & \quad &+ \quad & x {\langle {\mathbf{s}}_R, {\mathbf{H}} \rangle} &\quad &+\quad & {\langle z {\mathbf{y}}^n + z^2 {\mathbf{2}}^n, {\mathbf{H}}' \rangle} \\ + &\quad & \quad & + & \quad & \quad & + &\quad & \quad & \\ {\widetilde{e}} {\widetilde{B}} &\quad &= \quad & {\widetilde{a}} {\widetilde{B}} & \quad &+ \quad & x {\widetilde{s}} {\widetilde{B}} &\quad & \quad & \\ \shortparallel &\quad & \quad & \shortparallel & \quad & \quad & \shortparallel &\quad & \quad & \shortparallel \\ &\quad &= \quad & A & \quad &+ \quad & x S &\quad &+\quad & {\langle z {\mathbf{y}}^n + z^2 {\mathbf{2}}^n, {\mathbf{H}}' \rangle} - z{\langle {\mathbf{1}}, {\mathbf{G}} \rangle} \end{aligned} We can interpret the rows and columns similarly to the previous diagram: the sum of each column is a vector Pedersen commitment with left and right halves from the first and second rows respectively and blinding factor from the third row. The sum of all of the columns is a vector Pedersen commitment to $${\mathbf{l}}(x)$$ and $${\mathbf{r}}(x)$$ with synthetic blinding factor $${\widetilde{e}}$$.

To convince the verifier that $$t(x) = {\langle {\mathbf{l}}(x), {\mathbf{r}}(x) \rangle}$$, the prover sends $${\widetilde{e}}$$ to the verifier, who uses the bottom row to compute \begin{aligned} P &= -{\widetilde{e}} {\widetilde{B}} + A + x S + {\langle z {\mathbf{y}}^n + z^2 {\mathbf{2}}^n, {\mathbf{H}}' \rangle} - z{\langle {\mathbf{1}}, {\mathbf{G}} \rangle}\\ &= -{\widetilde{e}} {\widetilde{B}} + A + x S + {\langle z {\mathbf{1}} + z^2 {\mathbf{y}^{-n}} \circ {\mathbf{2}}^n, {\mathbf{H}} \rangle} - z{\langle {\mathbf{1}}, {\mathbf{G}} \rangle}; \end{aligned} if the prover is honest, this is $$P = {\langle {\mathbf{l}}(x), {\mathbf{G}} \rangle} + {\langle {\mathbf{r}}(x), {\mathbf{H}}' \rangle}$$, so the verifier uses $$P$$, $$t(x)$$ as inputs to the inner-product protocol to prove that $$t(x) = {\langle {\mathbf{l}}(x), {\mathbf{r}}(x) \rangle}$$.

# Inner-product proof

First, let’s observe that the prover can simply send vectors $${\mathbf{l}}(x)$$ and $${\mathbf{r}}(x)$$ and the verifier can check directly that the inner product $$t(x)$$ and commitment $$P$$ provided in the protocols 1 and 2 are correct. This will not leak information (the secret bits in these vectors are blinded), but will require us to transfer $$2n$$ scalars between a prover and a verifier.

To minimize the bandwidth cost we will use the inner-product argument protocol which enables us to prove indirectly and with $$O(log(n))$$ communication cost, that a given inner product $$t(x)$$ and a commitment $$P$$ are related as: \begin{aligned} t(x) &= {\langle {\mathbf{l}}(x), {\mathbf{r}}(x) \rangle} \\ P &= {\langle {\mathbf{l}}(x), {\mathbf{G}} \rangle} + {\langle {\mathbf{r}}(x), {\mathbf{H}}' \rangle} \end{aligned} To make the presentation cleaner, we will change the notation to one used specifically in the inner product argument which is not to be confused with the notation in the rangeproof protocol: \begin{aligned} {\mathbf{a}}, {\mathbf{b}} &\in {\mathbb Z_{p}^{n}}\\ {\mathbf{G}}, {\mathbf{H}} &\in {\mathbb G^{n}}\\ c &= {\langle {\mathbf{a}}, {\mathbf{b}} \rangle}\\ P &= {\langle {\mathbf{a}}, {\mathbf{G}} \rangle} + {\langle {\mathbf{b}}, {\mathbf{H}} \rangle} \end{aligned} Within the above definitions we need a proof of knowledge for the following relation: \begin{aligned} P &{}={}&& {\langle {\mathbf{a}}, {\mathbf{G}} \rangle} + {\langle {\mathbf{b}}, {\mathbf{H}} \rangle} \hspace{0.2cm} \wedge\\ c &{}={}&& {\langle {\mathbf{a}}, {\mathbf{b}} \rangle} \end{aligned} Let’s combine these two statements into one equation using an indeterminate variable $$w \in {\mathbb Z_{p}^{\times}}$$ and multiplying the second equation by an orthogonal generator $$B \in {\mathbb G}$$: \begin{aligned} P &{}={}&& {\langle {\mathbf{a}}, {\mathbf{G}} \rangle} + {\langle {\mathbf{b}}, {\mathbf{H}} \rangle}\\ &{}+{}&&\\ c w B &{}={}&& {\langle {\mathbf{a}}, {\mathbf{b}} \rangle} w B \end{aligned} Let’s simplify the resulting equation using the following definitions: \begin{aligned} k &= \lg n \\ P' &= P + cwB \\ Q &= wB \end{aligned} The equation becomes: $P' = {\langle {\mathbf{a}}, {\mathbf{G}} \rangle} + {\langle {\mathbf{b}}, {\mathbf{H}} \rangle} + {\langle {\mathbf{a}}, {\mathbf{b}} \rangle} Q$ The combined equation is useful because it will allow us to compress each vector in half and arrive to the same form. By doing such compression $$\lg n$$ times we will end up with an equation where both vectors are one-element long and we can simply transmit them to check the final equality directly.

If the prover can demonstrate that the above $$P'$$ has such structure over generators $${\mathbf{G}}$$, $${\mathbf{H}}$$ and $$Q$$ for all $$w \in {\mathbb Z_{p}^{*}}$$, then the original $$P$$ and $$c$$ must satisfy the original relation $$(P = {\langle {\mathbf{a}}, {\mathbf{G}} \rangle} + {\langle {\mathbf{b}}, {\mathbf{H}} \rangle} \wedge c = {\langle {\mathbf{a}}, {\mathbf{b}} \rangle})$$.

Let’s introduce an indeterminate variable $$u_k \in {\mathbb Z_{p}^{\times}}$$ and compress the vectors by adding the left and the right halves separated by the variable $$u_k$$: \begin{aligned} {\mathbf{a}}^{(k-1)} &= {\mathbf{a}}_L \cdot u_k + u^{-1}_k \cdot {\mathbf{a}}_R \\ {\mathbf{b}}^{(k-1)} &= {\mathbf{b}}_L \cdot u^{-1}_k + u_k \cdot {\mathbf{b}}_R \\ {\mathbf{G}}^{(k-1)} &= {\mathbf{G}}_L \cdot u^{-1}_k + u_k \cdot {\mathbf{G}}_R \\ {\mathbf{H}}^{(k-1)} &= {\mathbf{H}}_L \cdot u_k + u^{-1}_k \cdot {\mathbf{H}}_R \end{aligned} The powers of $$u_k$$ are chosen so they cancel out in the inner products of interest as will be shown below.

Let $$P_k = P'$$ and define $$P_{k-1}$$ using the same equation as for $$P_k$$, but using the compressed vectors: $P_{k-1} = {\langle {\mathbf{a}}^{(k-1)}, {\mathbf{G}}^{(k-1)} \rangle} + {\langle {\mathbf{b}}^{(k-1)}, {\mathbf{H}}^{(k-1)} \rangle} + {\langle {\mathbf{a}}^{(k-1)}, {\mathbf{b}}^{(k-1)} \rangle} \cdot Q$ Expanding it in terms of the original $${\mathbf{a}}$$, $${\mathbf{b}}$$, $${\mathbf{G}}$$ and $${\mathbf{H}}$$ gives: \begin{aligned} P_{k-1} &{}={}& &{\langle {\mathbf{a}}_L \cdot u_k + u_k^{-1} \cdot {\mathbf{a}}_R, {\mathbf{G}}_L \cdot u^{-1}_k + u_k \cdot {\mathbf{G}}_R \rangle} + \\ && &{\langle {\mathbf{b}}_L \cdot u^{-1}_k + u_k \cdot {\mathbf{b}}_R, {\mathbf{H}}_L \cdot u_k + u^{-1}_k \cdot {\mathbf{H}}_R \rangle} + \\ && &{\langle {\mathbf{a}}_L \cdot u_k + u^{-1}_k \cdot {\mathbf{a}}_R, {\mathbf{b}}_L \cdot u^{-1}_k + u_k \cdot {\mathbf{b}}_R \rangle} \cdot Q \end{aligned} Breaking down in simpler products: \begin{aligned} P_{k-1} &{}={}& &{\langle {\mathbf{a}}_L, {\mathbf{G}}_L \rangle} + {\langle {\mathbf{a}}_R, {\mathbf{G}}_R \rangle} &{}+{}& u_k^2 {\langle {\mathbf{a}}_L, {\mathbf{G}}_R \rangle} + u^{-2}_k {\langle {\mathbf{a}}_R, {\mathbf{G}}_L \rangle} + \\ && &{\langle {\mathbf{b}}_L, {\mathbf{H}}_L \rangle} + {\langle {\mathbf{b}}_R, {\mathbf{H}}_R \rangle} &{}+{}& u^2_k {\langle {\mathbf{b}}_R, {\mathbf{H}}_L \rangle} + u^{-2}_k {\langle {\mathbf{b}}_L, {\mathbf{H}}_R \rangle} + \\ && &({\langle {\mathbf{a}}_L, {\mathbf{b}}_L \rangle} + {\langle {\mathbf{a}}_R, {\mathbf{b}}_R \rangle})\cdot Q &{}+{}& (u^2_k {\langle {\mathbf{a}}_L, {\mathbf{b}}_R \rangle} + u^{-2}_k {\langle {\mathbf{a}}_R, {\mathbf{b}}_L \rangle}) \cdot Q \end{aligned} We now see that the left two columns in the above equation is the definition of $$P_k$$, while various cross terms on the right are separated from $$P_k$$ by an indeterminate variable $$u_k$$. Let’s group all terms with $$u^2_k$$ as $$L_k$$ and all terms with $$u^{-2}_k$$ as $$R_k$$: \begin{aligned} P_{k-1} &= P_k + u^2_k \cdot L_k + u^{-2}_k \cdot R_k\\ L_k &= {\langle {\mathbf{a}}_L, {\mathbf{G}}_R \rangle} + {\langle {\mathbf{b}}_R, {\mathbf{H}}_L \rangle} + {\langle {\mathbf{a}}_L, {\mathbf{b}}_R \rangle} \cdot Q\\ R_k &= {\langle {\mathbf{a}}_R, {\mathbf{G}}_L \rangle} + {\langle {\mathbf{b}}_L, {\mathbf{H}}_R \rangle} + {\langle {\mathbf{a}}_R, {\mathbf{b}}_L \rangle} \cdot Q \end{aligned} If the prover commits to $$L_k$$ and $$R_k$$ before $$u_k$$ is randomly sampled, then if the statement about compressed vectors is proven to be true, it will follow that the original statement about uncompressed vectors is also true with an overwhelming probability.

We can compress the resulting statement about $$P_{k-1}$$ using one more indeterminate variable $$u_{k-1}$$ in the same way as we used $$u_k$$ and arrive to even shorter vectors. We will continue doing so until we end up with vectors $${\mathbf{a}}^{(0)}, {\mathbf{b}}^{(0)}, {\mathbf{G}}^{(0)}, {\mathbf{H}}^{(0)}$$, each containing one item, and $$P_0$$ containing all accumulated cross-terms at each step: \begin{aligned} P_0 &= a^{(0)}_0 G^{(0)}_0 + b^{(0)}_0 H^{(0)}_0 + a^{(0)}_0 b^{(0)}_0 Q\\ P_0 &= P_k + \sum_{j=1}^{k} \left( L_{j} u_{j}^{2} + u_{j}^{-2} R_{j} \right) \end{aligned}

Rewriting the above with the definitions $$P_k = P' = P + cwB$$ and $$Q = wB$$ gives the final statement: $P + c w B = a^{(0)}_0 G^{(0)}_0 + b^{(0)}_0 H^{(0)}_0 + a^{(0)}_0 b^{(0)}_0 wB - \sum_{j=1}^{k} \left( L_{j} u_{j}^{2} + u_{j}^{-2} R_{j} \right)$

At this point the prover can transmit two scalars $$a^{(0)}_0$$ and $$b^{(0)}_0$$ to the verifier, so they check the final statement directly by computing both sides of the equation.

The resulting protocol has $$\lg n$$ steps of compression where the prover sends a pair $$(L_j,R_j)$$ of points at each step $$j = k\dots1$$. An additional and final step involves sending a pair of scalars $$(a^{(0)}_0,b^{(0)}_0)$$ and checking the final relation directly.

# Aggregated Range Proof

We want to take advantage of the logarithmic size of the inner-product protocol, by creating an aggregated range proof for $$m$$ values that is smaller than $$m$$ individual range proofs.

The aggregation protocol is a multi-party computation protocol, involving $$m$$ parties (one party per value) and one dealer, where the parties don't reveal their secrets to each other. The parties share their commitments with the dealer, and the dealer generates and returns challenge variables. The parties then share their proof shares with the dealer, and the dealer combines their shares to create an aggregated proof.

The Bulletproofs paper outlines two versions of multi-party computation aggregation. In the first approach, the inner-product proof is performed by the dealer, which requires sending the vectors used for the inner-product to the dealer. In the second approach, the inner-product proof is performed using multi-party computation, which sends less data but requires one round for each iteration of the inner-product protocol. We chose to implement the first approach because it requires fewer round trips between parties, which outweighed the slight message size savings of the second approach.

For more information on how the aggregation protocol works and is implemented, see the protocol notes.

The aggregated range proof has the same form as the individual range proof, in that the provers (the parties) still perform the same calculations to prove that $$t(x) = \langle \mathbf{l}(x), \mathbf{r}(x) \rangle$$ and that $$t_0, \mathbf{l}(x), \mathbf{r}(x)$$ are correct. The difference is that the challenge values are obtained from the dealer, which generates them by combining commitments from all the parties, and that the calculations of different parties are seperated by different powers of the challenge scalars $$y$$ and $$z$$.

We will explain how one piece of the aggregated proof is generated for party $$j$$, and then will show how all of the pieces for all of the $$m$$ parties can be combined into one aggregated proof.

## New notation for aggregated proofs

The subscript $${(j)}$$ denotes the $$j$$th party's share. For instance, $$v_{(j)}$$ is the $$v$$ value of the $$j$$th party; $$\mathbf{a}_{L, (j)}$$ is the $$\mathbf{a}_L$$ vector of the $$j$$th party; $$\mathbf{l}_{(0)}(x)$$ is the $$\mathbf{l}(x)$$ polynomial of party $$0$$.

We use pythonic notation to denote slices of vectors, such that $$\mathbf{G}_{[a:b]} = [\mathbf{G}_{a}, \mathbf{G}_{a+1}, \dots, \mathbf{G}_{b-1} ]$$.

$${\mathbf{G}_{(j)}}$$ is party $$j$$'s share of the generators $${\mathbf{G}}$$, or $${\mathbf{G}_{[j\cdot n : (j+1)n]}}$$, and $${\mathbf{H}'_{(j)}}$$ is party $$j$$'s share of the generators $${\mathbf{H}'}$$, or $${\mathbf{H}'_{[j\cdot n : (j+1)n]}}$$.

$$z_{(j)}$$ is a scalar offset that is unique to each party $$j$$, and is defined by $$z_{(j)} = z^j$$. $$\mathbf{y}^n_{(j)}$$ is a length $$n$$ vector offset that is unique to each party $$j$$. It is a slice into vector $$\mathbf{y}^{n \cdot m}$$, and is defined by $$\mathbf{y}^n_{(j)} = \mathbf{y}^{n \cdot m}_{[j \cdot n : (j+1) \cdot n]}$$

## Proving range statements with bit vectors

Party $$j$$ begins with a secret value $$v_{(j)}$$, and wishes to convince the verifier that $$v_{(j)} \in [0, 2^n)$$ without revealing $$v_{(j)}$$.

We want to make statements about $$v_{(j)}$$ using its bit vector representation, where the statements will be true if and only if $$v_{(j)}$$ is actually in the expected range. We will not reproduce the steps or explanation here since it is the same as in the proving range statements with bit vectors step of the single-value range proof. Here are the final statements for party $$j$$:

\begin{aligned} {\langle {\mathbf{a}}_{L, (j)}, {\mathbf{2}}^{n} \rangle} &= v_{(j)} \\ {\mathbf{a}}_{L, (j)} \circ {\mathbf{a}}_{R, (j)} &= {\mathbf{0}} \\ ({\mathbf{a}}_{L, (j)} - {\mathbf{1}}) - {\mathbf{a}}_{R, (j)} &= {\mathbf{0}} \end{aligned}

## Proving vectors of statements with a single statement

We want to combine the above three statements into a single statement for party $$j$$, as in the proving vectors of statements step of the single-value range proof. We will additionally use offsets $$\mathbf{y}^n_{(j)}$$ and $$z_{(j)}$$ that are unique to each party $$j$$. Since these challenge values are independent for each party, we can later merge the per-party combined statements into one statement for all $$m$$ parties.

First, we will combine each of the two vector-statements into a single statement using the verifier's choice of challenge value $$y$$ that is shared across all parties, and offset by vector $$\mathbf{y}^n_{(j)}$$:

\begin{aligned} {\langle {\mathbf{a}}_{L, (j)}, {\mathbf{2}}^{n} \rangle} &= v_{(j)} \\ {\langle {\mathbf{a}}_{L, (j)} - {\mathbf{1}} - {\mathbf{a}}_{R, (j)}, {\mathbf{y}}^{n}_{(j)} \rangle} &= 0 \\ {\langle {\mathbf{a}}_{L, (j)}, {\mathbf{a}}_{R, (j)} \circ {\mathbf{y}}^{n}_{(j)} \rangle} &= 0 \end{aligned}

The three resulting statements can then be combined in the same way, using the verifier’s choice of challenge value $$z$$ that is shared across all parties, and offset by scalar $$z_{(j)}$$ : \begin{aligned} z^{2} z_{(j)} \cdot v_{(j)} &= z^{2} z_{(j)} \cdot {\langle {\mathbf{a}}_{L, (j)}, {\mathbf{2}}^{n} \rangle} \\ &+ z \cdot {\langle {\mathbf{a}}_{L, (j)} - {\mathbf{1}} - {\mathbf{a}}_{R, (j)}, {\mathbf{y}}^{n}_{(j)} \rangle} \\ &+ {\langle {\mathbf{a}}_{L, (j)}, {\mathbf{a}}_{R, (j)} \circ {\mathbf{y}}^{n}_{(j)} \rangle} \end{aligned}

## Combining inner products

We combine the terms in the preceding statement into a single inner product, using the same technique as in the single-value range proof. We will not reproduce the math here since it is the same as in the combining inner products step of the single-value proof. Here is the end result:

\begin{aligned} \delta_{(j)}(y,z) &= (z - z^{2}) \cdot {\langle {\mathbf{1}}, {\mathbf{y}}^{n}_{(j)} \rangle} - z^{3} z_{(j)} \cdot {\langle {\mathbf{1}}, {\mathbf{2}}^{n} \rangle}\\ z^{2}z_{(j)} \cdot v_{(j)} + \delta_{(j)}(y,z) &= {\langle {\mathbf{a}}_{L, (j)} - z {\mathbf{1}}, {\mathbf{y}}^{n}_{(j)} \circ ({\mathbf{a}}_{R, (j)} + z {\mathbf{1}}) + z^{2} z_{(j)} \cdot {\mathbf{2}}^{n} \rangle} \end{aligned}

## Blinding the inner product

The prover chooses vectors of blinding factors $$\mathbf{s}_{L, (j)}, {\mathbf{s}}_{R, (j)}$$, and uses them to construct the blinded vector polynomials $$\mathbf{l}_{(j)}(x), \mathbf{r}_{(j)}(x)$$. We will not reproduce the steps or the explanation here since it is the same as in the blinding the inner product step of the single-value proof. Here are the final equations for the vector polynomials:

\begin{aligned} {\mathbf{l}}_{(j)}(x) &= ({\mathbf{a}}_{L, (j)} + {\mathbf{s}}_{L, (j)} x) - z {\mathbf{1}} & \in {\mathbb Z_p}[x]^{n} \\ {\mathbf{r}}_{(j)}(x) &= {\mathbf{y}}^{n}_{(j)} \circ \left( ({\mathbf{a}}_{R, (j)} + {\mathbf{s}}_{R, (j)} x\right) + z {\mathbf{1}}) + z^{2} z_{(j)} {\mathbf{2}}^{n} &\in {\mathbb Z_p}[x]^{n} \end{aligned}

## Proving that $$t(x)$$ is correct

Proving that $$t_{(j)}(x)$$ is correct means proving that $${\mathbf{l}}_{(j)}(x)$$, $${\mathbf{r}}_{(j)}(x)$$ are correctly formed, and that $$t_{(j)}(x) = {\langle {\mathbf{l}}_{(j)}(x), {\mathbf{r}}_{(j)}(x) \rangle}$$.

We can combine the statements about $$t_{(j)}(x)$$, $${\mathbf{l}}_{(j)}(x)$$, and $${\mathbf{r}}_{(j)}(x)$$ from all $$m$$ parties in the following manner:

\begin{aligned} t(x) &= \sum_{j=0}^{m-1} t_{(j)}(x)\\ {\mathbf{l}}(x) &= {\mathbf{l}}_{(0)}(x) || {\mathbf{l}}_{(1)}(x) || \dots || {\mathbf{l}}_{(m-1)}(x) \\ {\mathbf{r}}(x) &= {\mathbf{r}}_{(0)}(x) || {\mathbf{r}}_{(1)}(x) || \dots || {\mathbf{r}}_{(m-1)}(x) \\ \end{aligned}

We can add the $$t_{(j)}(x)$$ values together to create $$t(x)$$ instead of taking a random linear combination of $$t_{(j)}(x)$$ values, because each $$t_{(j)}(x)$$ is calculated with the $$\mathbf{y}^n_{(j)}$$ and $$z_{(j)}$$ challenge variables that are unique to that party $$j$$, so all of the $$t_{(j)}(x)$$ values will be offset from one another.

Now instead of having to do $$m$$ individual checks to prove that $$t_{(j)}(x)$$, $${\mathbf{l}}_{(j)}(x)$$, and $${\mathbf{r}}_{(j)}(x)$$ for all parties $$j$$ are correct, we can do the verification with one check:

\begin{aligned} t(x) \stackrel{?}{=} {\langle {\mathbf{l}}(x), {\mathbf{r}}(x) \rangle} \end{aligned}

We can do this check using the inner product proof, in the same way the single-value range proof uses the inner product proof.

## Proving that $$t_0$$ is correct

Proving that $$t_{0, (j)}$$ is correct requires first creating commitments to the variables, and then proving a relation over the commitments. For an explanation of how the commitments are created and how the relation is derived, see the proving that $$t_0$$ is correct step of the single-value range proof. The statement each party wants to prove is:

\begin{aligned} t_{(j)}(x) B + {\tilde{t}}_{(j)}(x) {\widetilde{B}} \stackrel{?}{=} z^2 z_{(j)} V_{(j)} + \delta_{(j)}(y,z) B + x T_{1, (j)} + x^{2} T_{2, (j)}\\ \delta_{(j)}(y,z) = (z - z^{2}) \cdot {\langle {\mathbf{1}}, {\mathbf{y}}^{n}_{(j)} \rangle} - z^{3} z_{(j)} \cdot {\langle {\mathbf{1}}, {\mathbf{2}}^{n} \rangle} \end{aligned}

If we combine all of the statements about $$t_{0, (j)}$$ from all of the $$j$$ parties by adding them together, then we get:

\begin{aligned} \sum_{j=0}^{m-1}t_{(j)}(x) B + \sum_{j=0}^{m-1}{\tilde{t}}_{(j)}(x) {\widetilde{B}} \stackrel{?}{=} z^2 \sum_{j=0}^{m-1} z_{(j)} V_{(j)} + \sum_{j=0}^{m-1} \delta_{(j)}(y,z) B + x \sum_{j=0}^{m-1} T_{1, (j)} + x^{2} \sum_{j=0}^{m-1} T_{2, (j)} \end{aligned}

We can combine the values and commitments by summing them directly. We can do this instead of having to take a random linear combination, because each party's values and commitments are already offset by the values $$\mathbf{y}^n_{(j)}$$ and $$z_{(j)}$$ that are unique to that party.

\begin{aligned} t(x) &= \sum_{j=0}^{m-1} t_{(j)}(x)\\ {\tilde{t}}(x) &= \sum_{j=0}^{m-1}{\tilde{t}}_{(j)}(x)\\ T_1 &= \sum_{j=0}^{m-1} T_{1, (j)}\\ T_2 &= \sum_{j=0}^{m-1} T_{2, (j)}\\ \delta(y,z) &= \sum_{j=0}^{m-1} \delta_{(j)}(y,z)\\ \end{aligned}

We can plug the equation for $$\delta_{(j)}(y,z)$$ into the calculation for $$\delta(y,z)$$:

\begin{aligned} \delta(y, z) &= (z - z^{2}) \cdot \sum_{j=0}^{m-1} {\langle {\mathbf{1}}, {\mathbf{y}}^{n}_{(j)} \rangle} - z^{3} \sum_{j=0}^{m-1} z_{(j)} \cdot {\langle {\mathbf{1}}, {\mathbf{2}}^{n \cdot m} \rangle}\\ \end{aligned}

Since we know that $$\mathbf{y}^n_{(j)} = \mathbf{y}^{n \cdot m}_{[j \cdot n : (j+1) \cdot n]}$$, we can simplify $$\delta(y, z)$$:

\begin{aligned} \delta(y, z) &= (z - z^{2}) \cdot ( {\langle {\mathbf{1}}, \mathbf{y}^{n \cdot m}_{[0 : n]} \rangle + \langle {\mathbf{1}}, \mathbf{y}^{n \cdot m}_{[n : 2 \cdot n]} \rangle + \dots + \langle {\mathbf{1}}, \mathbf{y}^{n \cdot m}_{[(m-1) \cdot n : m \cdot n]} \rangle}) - z^{3} \sum_{j=0}^{m-1} z_{(j)} \cdot {\langle {\mathbf{1}}, {\mathbf{2}}^{n \cdot m} \rangle} \\ &= (z - z^{2}) \cdot {\langle {\mathbf{1}}, \mathbf{y}^{n \cdot m} \rangle} - z^{3} \sum_{j=0}^{m-1} z_{(j)} \cdot {\langle {\mathbf{1}}, {\mathbf{2}}^{n \cdot m} \rangle} \\ \end{aligned}

Now instead of having to do $$m$$ individual checks to prove that $$t_{0, (j)}$$ for all parties $$j$$ are correct, we can do the verification with one check using the combined values:

\begin{aligned} t(x) B + {\tilde{t}}(x) {\widetilde{B}} \stackrel{?}{=} z^2 \sum_{j=0}^{m-1} z_{(j)} V_{(j)} + \delta(y,z) B + x T_{1} + x^{2} T_{2},\\ \delta(y,z) = (z - z^{2}) \cdot {\langle {\mathbf{1}}, {\mathbf{y}}^{n \cdot m} \rangle} - z^{3} \sum_{j=0}^{m-1} z_{(j)} \cdot {\langle {\mathbf{1}}, {\mathbf{2}}^{n \cdot m} \rangle}\\ \end{aligned}

Since we know that $$z_{(j)} = z^j$$, we can rewrite the equation as follows:

\begin{aligned} t(x) B + {\tilde{t}}(x) {\widetilde{B}} \stackrel{?}{=} \sum_{j=0}^{m-1} z^{j+2} V_{(j)} + \delta(y,z) B + x T_{1} + x^{2} T_{2},\\ \delta(y,z) = (z - z^{2}) \cdot {\langle {\mathbf{1}}, {\mathbf{y}}^{n \cdot m} \rangle} - \sum_{j=0}^{m-1} z^{j+3} \cdot {\langle {\mathbf{1}}, {\mathbf{2}}^{n \cdot m} \rangle}\\ \end{aligned}

## Proving that $${\mathbf{l}}(x)$$, $${\mathbf{r}}(x)$$ are correct

Proving that $${\mathbf{l}}_{(j)}(x)$$, $${\mathbf{r}}_{(j)}(x)$$ are correct requires first creating commitments to the variables, and then proving a relation over the commitments. For an explanation of how the commitments are created and how the relation is derived, see the proving that $${\mathbf{l}}(x)$$, $${\mathbf{r}}(x)$$ are correct step of the single-value range proof. The statement that each party wants to prove is:

\begin{aligned} {\langle {\mathbf{l}}_{(j)}(x), {\mathbf{G}_{(j)}} \rangle} + {\langle {\mathbf{r}}_{(j)}(x), {\mathbf{H}'}_{(j)} \rangle} \stackrel{?}{=} -{\widetilde{e}_{(j)}} {\widetilde{B}} + A_{(j)} + x S_{(j)} - z{\langle {\mathbf{1}}, {\mathbf{G}_{(j)}} \rangle} + {\langle z \mathbf{y}^{n}_{(j)} + z^2 z_{(j)} {\mathbf{2}}^n, {\mathbf{H}'}_{(j)} \rangle} \end{aligned}

If we combine all of the statements about $${\mathbf{l}}(x)$$, $${\mathbf{r}}(x)$$ from all the $$j$$ parties by adding them together, then we get:

\begin{aligned} \sum_{j=0}^{m-1}{\langle {\mathbf{l}}_{(j)}(x), {\mathbf{G}_{(j)}} \rangle} + \sum_{j=0}^{m-1}{\langle {\mathbf{r}}_{(j)}(x), {\mathbf{H}'}_{(j)} \rangle} \stackrel{?}{=} -\sum_{j=0}^{m-1}{\widetilde{e}_{(j)}} {\widetilde{B}} + \sum_{j=0}^{m-1}A_{(j)} + x \sum_{j=0}^{m-1}S_{(j)} - z \sum_{j=0}^{m-1}{\langle {\mathbf{1}}, {\mathbf{G}_{(j)}} \rangle} + \sum_{j=0}^{m-1}{\langle z {\mathbf{y}^n_{(j)}} + z^2 z_{(j)} {\mathbf{2}}^n, {\mathbf{H}'_{(j)}} \rangle} \end{aligned}

We can simplify this expression by making a few observations. We know that:

\begin{aligned} &{\mathbf{l}}(x) &{}&=&{}& {\mathbf{l}}_{(0)}(x) & {} &||& {} & {\mathbf{l}}_{(1)}(x) & {} &||& {} & \dots & {} &||& {} & {\mathbf{l}}_{(m-1)}(x) \\ &{\mathbf{r}}(x) &{}&=&{}& {\mathbf{r}}_{(0)}(x) & {} &||& {} & {\mathbf{r}}_{(1)}(x) & {} &||& {} & \dots & {} &||& {} & {\mathbf{r}}_{(m-1)}(x) \\ &{\mathbf{G}} &{}&=&{}& {\mathbf{G}}_{(0)} & {} &||& {} & {\mathbf{G}}_{(1)} & {} &||& {} & \dots & {} &||& {} & {\mathbf{G}}_{(m-1)} \\ &{\mathbf{H}'} &{}&=&{}& {\mathbf{H}'}_{(0)} & {} &||& {} & {\mathbf{H}'}_{(1)} & {} &||& {} & \dots & {} &||& {} & {\mathbf{H}'}_{(m-1)} \end{aligned} \begin{aligned} \mathbf{y}^n_{(j)} &= \mathbf{y}^{n \cdot m}_{[j \cdot n : (j+1) \cdot n]} \\ z_{(j)} &= z^j \end{aligned}

Therefore, we can simplify the following statements:

\begin{aligned} \sum_{j=0}^{m-1}{\langle {\mathbf{l}}_{(j)}(x), {\mathbf{G}_{(j)}} \rangle} &= {\langle {\mathbf{l}}_{(0)}(x), {\mathbf{G}}_{(0)} \rangle} + {\langle {\mathbf{l}}_{(1)}(x), {\mathbf{G}}_{(1)} \rangle} + \dots + {\langle {\mathbf{l}}_{(m-1)}(x), {\mathbf{G}}_{(m-1)} \rangle}\\ &= {\langle {\mathbf{l}}_{(0)}(x) || {\mathbf{l}}_{(1)}(x) || \dots || {\mathbf{l}}_{(m-1)}(x), {\mathbf{G}}_{(0)} || {\mathbf{G}}_{(1)} || \dots || {\mathbf{G}}_{(m-1)} \rangle} \\ &= {\langle {\mathbf{l}}(x), {\mathbf{G}} \rangle} \\ \sum_{j=0}^{m-1}{\langle {\mathbf{r}}_{(j)}(x), {\mathbf{H}'}_{(j)} \rangle} &= {\langle {\mathbf{r}}_{(0)}(x), {\mathbf{H}'}_{(0)} \rangle} + {\langle {\mathbf{r}}_{(1)}(x), {\mathbf{H}'}_{(1)} \rangle} + \dots + {\langle {\mathbf{r}}_{(m-1)}(x), {\mathbf{H}'}_{(m-1)} \rangle} \\ &= {\langle {\mathbf{r}}_{(0)}(x) || {\mathbf{r}}_{(1)}(x) || \dots || {\mathbf{r}}_{(m-1)}(x), {\mathbf{H}'}_{(0)} || {\mathbf{H}'}_{(1)} || \dots || {\mathbf{H}'}_{(m-1)} \rangle}\\ &= {\langle {\mathbf{r}}(x), {\mathbf{H}'} \rangle} \end{aligned}

We can combine the values and commitments from all the $$m$$ parties by summing them directly:

\begin{aligned} {\widetilde{e}} &= \sum_{j=0}^{m-1} {\widetilde{e}_{(j)}} \\ A &= \sum_{j=0}^{m-1} A_{(j)} \\ S &= \sum_{j=0}^{m-1} S_{(j)} \\ \end{aligned}

With these observations, we can simplify the combined $$m$$-party statement about $${\mathbf{l}}(x)$$ and $${\mathbf{r}}(x)$$ into:

\begin{aligned} {\langle {\mathbf{l}}(x), {\mathbf{G}} \rangle} + {\langle {\mathbf{r}}(x), {\mathbf{H}'} \rangle} \stackrel{?}{=} -{\widetilde{e}} {\widetilde{B}} + A + x S - z{\langle {\mathbf{1}}, {\mathbf{G}} \rangle} + z{\langle {\mathbf{y}^{n \cdot m}}, {\mathbf{H}'} \rangle} + \sum_{j=0}^{m-1} {\langle z^{j+2} \cdot {\mathbf{2}}^n, {\mathbf{H}'}_{[j \cdot n : (j+1) \cdot n]} \rangle} \end{aligned}

1. Generally, condition $$x=0 \vee y=0$$ can be expressed as $$x \cdot y = 0$$, as the product can be zero if and only if at least one of the terms is zero. This trick allows implementing logical OR with any number of terms.

2. This is because the polynomial in terms of $$y$$ is zero at every point if and only if every term of it is zero. The verifier is going to sample a random $$y$$ after the prover commits to all the values forming the terms of that polynomial, making the probability that the prover cheated negligible. This trick allows implementing logical AND with any number of terms.

3. The blinding factor is synthetic in the sense that it is synthesized from the blinding factors of the other commitments.